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Full text of "Miscellanea curiosa. Containing a collection of some of the principal phaenomena in nature, accounted for by the greatest philosophers of this age; being the most valuable discourses, read and delivered to the Royal Society, for the advancement of physical and mathematical knowledge. As also a collection of curious travels, voyages, antiquities, and natural histories of countries; presented to the same society"

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— Mifcellanea Curtofa : 


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CONTAINING A 


COLLECTION 


Of fome of the Principal 


PHENOMENA 
NATURE 


Accounted for by the Greateft Philo- 
fophers of this Age ; 
BEING THE 


Moft Valuable Difcourfes, Read and Deliver’d to 
the Royal Society, for the Advancement of Phyfi- 
jel and Mathematical Knowledge. 


VOL. I. 
To which . added, 


The LAWS of Stereographick Projection, 
Laid down and Demonitrated, by Fa. 
Bp Piedgfor, F.R. 5. 


LONDON, 


Printed by F. AZ for R. Smith, at the Bible, under the 
— ~Piarza of the Royal- “Exchange i in Cornhill. 1708. 


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Calculation of the Credibility of Hu- 
fh mane Teftimony. | Page 1 
A Letter from the Reverend Dr. Wallis, Pro- 
- felfor of Geometry in the Univerfity of Oxford, 
and Fellow of the Royal Society, London, to 
_ Mr. Richard Norris, concerning the Colle- 
_ Gion of Secants ; and the true Divifion of the 
 Meridians in the Sea-Chart. Ms, 9 
‘An eafie Demonftration of the Analogy of the 
_ Logarithmick, Tangents to the Meridian Line 
or fum of the Secants 5 with various Methods 
"for computing the fame to the utmoft Exattnefs, 
 byE. Halley. _ “20 
‘A moft compendious and facile Method for Con- 
 ftrutting the Logarithms, exemplified and de@ 
monftrated from the Nature of Numbers, withe 
out any regard to the Hyperbola, with a {pee- 
dy Method for finding the Number from the 
Logarithn: given. By KE. Halley. 37 
“A Solution given by Mr. John Collins, of 4 
~ Chorographical Problem, Propofed by Richard | 
-. Townley, E/7; oa uel 
The Solutions of three Chorographic Problems, by 
4 Member of the Philofophical Society of 
Oxford. ne | 8 
| t “An Arithmetical Paradox, concerning the Chances 
of Lotteries by ah os cies Francis Rob- 
Ja 2 


: erts 


aa 
ee 


the CON TEN Pa 3 
_.etts, £/qs., Fellow of the. R:S.- - ae 65. 
AA New, Exatt and Ealie Method, of finding the 
_ Roots of any Equations generally, and that 

without any previous Reduttion, By Edm. 
_ p&lalley.. = : a oe 712 
AA Differtation concerning the Comftruttion of So- 
‘lid Problems, or Equations of the third or 
fourth Power, by the help of one (given) Para- 
bola and a Circle. By Edmund Halley. 89 
‘A Difcourfe concerning the Number of Roots, 
in Solid and Biquadratical Equations, as alfo 
of the Limits of them. ByE. Halley. 101 
Some Iluftrious Specimens of the Dottrine of 
_ Eluxions, or Examples by which w clearly 
fheton the Ufe and Excellency of that Method 
in folving Geometrical Problems, By Ab. 
_ De Moivre. | 128 
A Method of Squaring fome Sorts of Curves, 
Or Reducing them to more fimple Curves. By 
A. De Moivre, 2.5.5. a AO 
Tio Problems « VIZ. concerning the Solid of 
 Leaft Refiftance, and the Curve of Swifteft 
Defeent. Salad by J. Craig. 159 
The Quadrature of the Logarithmical Curve. 
By j. Craig. ys rte mae 2 
A Theorem concerning the Prp>-tion of the Time 
“that a heavy Body [pends in defcending thro’ 
a right Line joining two given Points, to the 
(fhorteft) Tze, in which it paffes from the 
one to the other of thefe Points, by the Arch 


Of 4 Cyelord, 8. | 168 
An Extrat of a Letter fromthe Reverend Dr. 
John Wallis, to Richard Waller, E/g;. Se- 
cretary to the Royal Society, concerning the 
Spaces in the Cycloid, which are perfectly 
| Buadrables : 171 


, ee BE lar * 
hy meets 


me fhe CON PEN'ES. 
Fhe Quadrature of a Portion of the Epycloid. By 
eaar  Cafwell.: é ATF 
A General Propofition, fhewing the Dimenfion of 
the Areas iv all thofe kinds of Curves which 
are defcrib’d by the Equable Revolution of .2 
Circle upon any Bafis, either a Rettilineal or 
a Circular one. By Edm. Halley. 177 
A Method of Raifing an infinite Multinomial to 
_any given Power, or Extratting any given Root 
of the fame. By Mr. A. De Moivre. 183 
A Method of Extratting the Root of an Infinite 
Equation. By A. De Moivre, F.R.S. 191. 
An Experiment of the Refrattion of the Air, © 
made at the Command of the Royal Society, 
March 28. 1699. By J. Lowthorp, 4.124.196 
A Difcourfe concerning a Method of Difcovering 
the True Moment of the Suns Ingrefs into the 
_ Tropical Sines. By BE. Halley. 202 
AA Seale ef the Degrees of Heat. 215) 
“The Properties of the Catenaria. By David 
. Gregory, AZ, D. Savilian Profeffor of Aftro- 
nomy, and F.R.S. 219 
Of the Quadratures of Geometrically irrational - 
Figures, By }. Craig. 251! 
Concerning the Apparent Magnitude of the Sun 
~ and Moon, or the apparent diftance of two 
Stars when nigh the Horizon, and when high- 
er elevated. 263 
The Sentiments of the Reverend and Learned Dr. 
_* John Wallis R. S. Soc. upon the aforefaid 
Appearance, communicated ia a Letter to the 
Publifher. e275 
A Demonftration of an Error committed by com- 
mon Surveyors in comparing of Surveys,taken at 
long Intervals of Time, arifing from the Vari- 
ation of the Magnetick, Needle, by William 
Ry ee ee te Moly- 


a 


7 arom 


SN eee TR Sree Oa st SED 
- ~ = 


The CONTENTS. — 
Molyneux. E/q,; F. R. S. oop 2. 
‘A Propofal concerning the Parallax of the fixed 
- Stars, in Reference tothe Earths Annual Orb. 
In feveral Letters of May the 2d. June 29. 
and July 20. 1693. from Dr. John Wallis 

to William Molyneux Efg, 


292 
Why Bodies diffolved in Menjftrua Specifically 


lighter than themfelves, fwimtherein? 300 
Of the weight of a Cubic foot of divers grains, 
&c. wyd ina Veffel of well-feafowd Oak, 
whofe concave was an exatt cubic foot. By 
the direttion of the Philofophical Society at 
Oxford. 308 


“AA Letter of Dr. Wallis to Dr. Sloane, concern-~ 


ing the Generation of Hail,and of Thunder and 


Lightning, and the Effetts thereof. 315 
A Synopfis of the Aftronomy of Comets. I 


A Geometrical Differtation Concerning the Rain- 
bow iz which (by a dirett Method) is fhewn 
how to fiad the Diameter of each Bow, the Pro- 
portion of the Refraction being given: Together 
~ with the Solution of the Inverfe Problem, or 
bow to find the Ratio of the Refrattion, the 
Diameter of the Iris being given. By Edm- 
Halley, F. R. 5. : "25 


+ 


Tabella Poteftatum. 


$ | t uz Ww 3 : y 
L 27 ol a’-+ol af e-l-2ail a’ ¢ e-4-351 a* e+-351 aett-oil a%e% 71 acti’ 
hz&—kaot-6k a’ e-|-15k a* ee ey ee ka e-}. k e& 
hzi hash at e-t-1oha? e e-f-10ha? e-- sha eh e? 
getagattag a et Opa? cel aga er g 
friafa-sfa eq 3fa ee fe 
 dzt=da’trada el dee 
czwmcoa+ ce 


\ 


This refers to Page 80 in this Volume. 


ADVERTISE MENT. 


". 'There is in the Prefs and will Speedily — 
be publifh’d, A Collection of the Travels, 
Antiquities and Natural Hiftoriesof Coun- © 
tries, as they have been deliver’d in to 
the Royal Society; collected from the: 
Philofophical TranfaCtions into one Voe 
fume in Oftavo. ‘a 


— Mifcellanea Curiofa. 


PART IL. 


A Calculation of the Credibility of 
5 — Humane Tefiimony. _ 


Oral Certitude "Ab/olute,is that in which 
the Mind of Man entirely acquief 
ed . ces, requiring no further Affurance ‘ 
As if one in whom I abfolutely confide, fhall 
bring me word of 12060/. accruing to me by 
Gift, or 4 Ship’s Arrival, and for which there- 
fore I would not give the leaft valuable Con- 
fideration to be Enfur’d. | 
Moral Gertitude Tacompleat, has its feveral 
Degrees to be eftimated by the Proportion it 
‘bears to the Ab/folure. As if one in whoml 
have that degree of Confidence, as that I would 
“not give above One in Six to be enfur’d of the 
‘trath of what he fays, fhall inform me, as a- 
‘bove, concerning 1200/. I may then reckon — 
that Ihave as good as the Abfolute Certainty 
of a 1000 /. or five fixths of Abfolute Certainty 


for the whole Summ. , 
r 5 Bs nl , The 


mes a 
ss i 


2 — Mifcellanea Curtofa. 

The Credibility of any Reporter is to berated — 
(1) by bis Jvtegrity or Fidelity; and (2) by his” 
Ability: and a double Ability is to be confider- 
ed; both that of Apprebending what is deliver’d, 
and alfo of Retaining it afterwards,. till it be 
tranfinikted. (4) F SAS VR aya: 

‘ What follows concerning the Degrees of 
© Credibility, is divided into Four Propofitions. 
‘The Two Firft, refpe@ the Reporters of the 
¢ Narrative; as they either Tranfinit Succe/five- 
“ly, or Atteft Concurrently : the Third, the Sub- — 
‘ veft of it; as it may confift-of feveral Articles: — 
© and the Fourth, joins thofe three Confiderati- 

‘ ons together, exemplifying them in Oral and 


# 


© in Written Tradition: 


PR OPS PE: 


Concerning, rhe Credibility of a Report, made by 
‘Single Succeflive Reporters, who are equally Cre- 
dible. ; 


_ Let their Reports have, each of them, five. 
Sixths of Certainty ; and let the firft Reporter. 
give me a Certainty of 1000/. in 1200 /. it is, 
plain, that the Second Reporter, who delivers. 
that Report, will give me the Certainty but of 
éths of that 1000 /. or the 3th of ths of the. 
full Certainty of the whole 12002... .And fo.a 
Third Reporter,who has it from the fecond,will 
tranfinit to me but zths of that Degree of Cer- 
tainty, the Second would have deliver’d me, 


a) a i s 7 z | 

. That is, if, 4, be put for the Share of Affu-_ 

rance a fingle Reporter gives me; and, c, for, 

that which 18 wanting to make shat Alfurance . 

gompleat; and 1 therefore fuppos’d to have — 
A 


Og ae me 
ie 

: ae 

a 


 Mifeellaiew Curiofa. 2 


& : : 

oC Certainty from the Firft Reporter ; I 

— gt : Aa. . 

fhall have’ from ‘thé Second,—=='; from the 
os bee a” a+” 


Third, gers", 


»; And accordingly, if, 2, be == 100, and c—=6) 
(the number of Pounds that an 1oo/. put out 
-t0 Intereft,. brings in at the Year’s.end;.) and 
-comfequently my, Share of Certainty from One 
‘Reporter, -be ==i5< 5 -which is the, prefent va- 
due of any Summ to be paid a Year hence: The 
Proportion of Certainty coming to me froma 
Second, will be $2 multiplyed by +3% Gyvhich 
is.the, prefent: Value of Mony to be paid after 
two-Years;,) and that from.a Third-hand. Re- 
‘porter, <= iar «thrice multiplied into it felf ; 
‘the Value of Mony payable at the end of 
Meee Beats) OC. ks 


YS "3° Eorollary. 


~ And ‘therefore, as at the Rate of 6 per Cent. 
Intereft, the prefent Value of any Summ pay- 

able after Twelve Years, is-but half the Summ 
So if the Probability or proportion of Certi- 
anes, tranfmitted by each Reporter, be ize; 

the Proportion of Certainty after Twelve fuch 
_Tranfmiffions, will be but as a half; and it will 
‘grow by that Time an equal Lay, whether the 
peat be true or no. Inthe fame manner, if 
‘the Proportion of Certainty be fet at ¥25 it 
will come to half from the 7orh Hand: And if 
a tea) from the 695th. | 


it 


gaia Po Be PROP. 


43 Mifcellanea Curiofa. 


PROP? at 
Concerning Concurrent Teftificatzons. 


If Two Concurrent Reporters have, each of 
them, as ¢ths of Certainty ; they will both give 
me an Aflurance of 2iths, or of 35 to one: If 
Three ; an Aflurance of 312, or of 215 to 
one. | ' 

For if one of them gives a Certainty for 
1200 1. as of 3ths, there remains but an Aflu- 
rance of {th, or of 200/. wanting to me, for 
the whole. And towards that the Second At- 
tefter contributes, according to his Proportion 
of Credibility: That is to ths of Certainty be- 
forehand, he adds ths of the th which was 
wanting: So that there is now wartting but 
sth of a &th, that is 3th; and confequently I 
have, from them both, 34ths of Certainty: So 
from Three, 233, Gc. age 3 
That is, if the firft Witnefs gives me — 
a--C 


of Certainty, and there is wanting of it 


Cy 

AKC 5 

the Second Attefter will add “— of that £5 
a-~c a*Kc 5 


and confequently leave nothing wanting but 


c ’ a c? seeks 
= of that i == ee like: man- 


oy ac 2 


ner the third Attefter adds his 2— of that 


.2 


e / ce a Stes 
» and leaves wanting only ——  -@ce. © 


Corol- 


Pe. 


Mifcelonea Curtofa. * 


. } 9195/1. . Corollary. : 

Hence it follows, that ifa fingle Witnefs 
fhould be only fo far Credible, as to give me 
the Half of a full Certainty ; the Second ofthe 
fame Credibility, would (joined with the firft) 
give me 3ths; a Third, gths, cc. So that the. 
Coatteftation ofa Tenth,would give me 3: 4ths 


of Certainty ; and the Coatteftation of aT wen- 


tieth, to35223 or above Two Millions to one, 


PRO P. 1h. 

Concerning the Credit of a Reporter for a Particu- 
lar Article of that Narrative, for the whole of 
which he is Credible in a certain Degree. 


Let there. be Six Particulars of a Narrative 


~ equally remarkable : If he to whom the Report 
vis given, has %ths of Certainty for the whole, 


--or Summ, of them; he has 35 to one, againft 
the Failure in any One certain Particular. 

» For he has Five to One, there will be no 
Failure atall. And ifthere be, he has yet a- 


nother Five to One, that it falls not upon that 


-fingle Particular of the Six. That is, he has 


4ths of Certainty for the whole: and of the seh 


wanting, he has likewife $rhs, or ,irhs of the 


_. whole more ; and thereforethat there will be 


no Failure in that fingle Particular, he has 


_ gths and $4ths of Certainty, or 45 of it. 


Bag 
a5 


Tn General, if <—-be the Proportion of Cer- 


. i - 
_ tainty for the whole; and ——— be the chance 


> of the reft of the particular Articles m, againit 


B 3 fome 


te AP ae Ag i piiraiuiaeah aie. nie 


ee: MifeeNanea Cui 


fome one, or more of them 7; there will be no- 
thing wanting toan abfolute Certitude ,againit — 
the not failing 10 sp few pe Articles, 2, a 


Ce g te Pies er iy re» 
jails meme te {/) i Vee 


marhaneacthe r ay aT 


EON ee eee 


PROP. Wwe 


Concerning the Truth of es Oral or Written 
Tradition, (in Whole, or in Part,) Succeflively- 
tranfinitted, and alfa Coattelted by feveral Suc- 
ceffions of Lage, | 
ae 1) Suppofing. the ‘Tranfinidfidn oh: an a Oral 

and Narrative to be fo. performed by. a Succef- - 

fon of Single Men, or joined in Companies, as 
othatveach: Trantinit a } after the “Narrative 
has ‘been! kept ‘for Tweaty. Years, impairs the 

Credit of ita /th part ; and-that confequently 

‘at the Twelfth: Hand; oratrthesendiiof. 240 - 

Years, its certainty is redaced to a: Half; and 

there grows then‘an even Lay (by the Corollary 

of tke fecond Propofiriar) againft the Truth of the 

Relation | Vet if we farther. fuppofe; thatthe 

-fame Relation is Coatteltet by Nine other feve 
yal Succeflions,tranfinitting alike each of them ; 
the Credibility of it when they are all found:to 
agree; wall (by the Corollary of the firft Propofition) 
be as 4333. or Certainty, or’ above a Thoufand 
to one: and if we ‘fuppofe aCoatteftation\ of 
| Ninetcen, the Credibility ei it Nie be, as a~ 
-bove' Two Millions ‘to’ One-- aD af 
(2) In Oral Tradition as a “Sinate Mah is 
fabject to much Cafuality, fo a Company of 

Men cannot be fo eafily fuppos’d to join; and 

therefore: the Credibility “_ thsi: aera 

ae E «eb Ne ts. 


i — Mifcellanea Curiofa. m7 
' 43ths,may poflibly be judged too high a Degree 
for an Oral Conveyance, to the diftance of 
Twenty Yeats. But in Written Tradition, the 
‘Ghances againft the Truth or Confervation‘of 
a fingle Writing, are far lefs, and feveral'Co- 
‘pies may alfo be eafily fippos’d to concur ;and 
thofe fince the Invention of Printing exactly 
the fame: feveral’ alfo' diftin® ‘Succeffions~ of 
“fach Copies may be as: well fuppos’d, taken by 
‘different Hands, and preferv’d in different 
‘Places or Languages. pre: sik te 
‘And therefore it Oral Tradition by anyone 
‘Man or Company of Men might be fuppos’d 
to be Credible, after Twenty Years at ‘2zhs 
of Certainty ; or but °,ths; or $ths: a' Writ- 
ten Tradition may be well imagin’d to conti- 
nue, by the Joint Copies that may be taken of 
it for one Place, (like the feveral Copies of the 
fame Impreffion} during the fpace of a 100, if 
not 200 Years ; and to be then Credible at 
724¢hs of Certainty, or at the Proportion of a 
Hundred to one. And then, feeing that the 
Succeflive Tranfmiffions of this 33° of Certain- 
ty, will not diminifh it to a Half, until it paf- 
des the. Sixty. nioth Hand ;..(forit..awill-benear 
Seventy Years before the Rebate of Mony, at 
that Intereft, will fink it to half: ) It is plain, 
that written Tradition, if preferv’d but by a 
fingle Succeflion of Copies, will not lofe half of 
its full Certainty, until 70 times a Hundred Cif 
not two Hundred) Years are paft; that is, Se- 
ven Thoufand, if not Fourteen thoufand Years; 
_and further, that, if it be likewife preferv’d 
by Concurrent Succeffions of. {uch Copies, its 
ccpbeing at that Diftance may be even en- 
-dreas’d, ahd grow far more certain from the 
feveral agreeing Deliveries at the end of Se- 
B 4. venty 


8 Mifcetlanea Curtofa. 
venty Succeffions, than it would be at the very — 
firft from either of the Single Hands. 4 
(3) Laftly,in ftating the Proportions of Cre- 
‘dibility for any Part or Parts of a Copy, it may 
_be obfery’d ; that in an Original not very long, 
good Odds may be laid by a careful Hand,that © 
the Copy fhall not have fo much as a Literal 
Fault: But in one of greater Length,that there 
may be greater Odds againft any Material Er- 
ror, and fuch as fhall-alter the Senfe; greater 
yet, that the Senfe fhal] not be alter’d in any 
confiderable Points; and ftill greater, if there 
be many of thofe Points, that the Error lights 
not upon fuch a fingle Article; as in the Third 

Propofition. a Hl hi 


| Mifcellanea Curiofa. —g 


A Letter from the Rewereni Dr. 
_ Wallis, Profeflor of Geometry zx 

_ the Univer fity of Oxford,and Fel- 
opi the Royal Society, London, 
_ to Mr. Richard Norris, concern- 
ing the Collection of Secants ; ; and 
: the true Divifion of the Mer idians 
_ an the Sea-Chart. 


N old enquiry, (about the Sum or Aggre- 

gate of Secants) having been of late mo- 

yed a-new ; I have thought fit to trace it from 

_ its Original : with fuch folution as feems pro- 

per to it: Beginning firft with the general 

Preparation ; and then applying i it to the Parti- 
cular Cafe. 


J : General Preparation. 


ai bi “Beeaufe Curve lines are not fo eafily ma- 


-naged as Straight lines: the Ancients, when 
they were to confider of Figures terminated 
(at leaft on one fide) bya ‘Curve line (Con- 
‘vex or Concave) as AFKE; Fig.1.2. Tab.1. did 
oft make ufe of fome fach expedient as this 


following, (but diverfly varied as occafion re- . 


quir’d.) Namely, 
2. By Parallel. Straight. lines, as AF, BG, 
CH, &c.. (at, equal or. unequal diftances, as 
there was occafion,) they parted it into fo ma- 


“ny: 


ao Mifcetanea Curiofa. 
ny Segments as they thought fit; (or fu ippofed 
at to-be fo parted)" 

3. Thefe Segments were fo many manting one, 
as(was the number of thofe Parallels. 

"4. To each of thefe Parallels, gta one ; 
they fitted Parallelograms, of fuch breadths as 
were the Intervals (équal or unequal) between 
each of them, (refpectively) and the next fol- 
dowing. Which formed an Adfcribed Figure 
madet up of thofe Parallelograms. 1) 
\..§- And,.if they, began with \the Greateft 
Gid therefore negle@ed.the leaft) fuch Figure 
was. Circumfcribed, (as Rig) rt.) and therefore 
Bigger than the Curvilinear propofed.. 

. If with the Leaft (negle@ting the great- 
ay . the Figure was Infcribed (as Fig, a.) 
vant therefore hefs than that propofed- 

vg. Butpasethe amber of Segments wit in- 
weed {ets (aiid thereby ‘their breadths' diminifh- 
ag ): the difference of the Cireumferibed from 
ithe Infcribed (and therefore of either ‘from 
that propofed) did continually decreafe, fo as 
at laft to be lefS than any affigned.-1)2 15.89 

8. On which oy, Evene! their Method 
of Exhauftions.: 

9. In cafes heen the Breadth of the Pa- 
rallelograits,. or Intervals of the'Parallels, is 
' mot to be confidered, but their Iength only ; 
(or, which is‘much: the fame; ‘wherethe Inter- 
yals/are'all the fame, and eachreputed ="1.) 
‘Archimedes. Cinftead oF Inferibed®a nd -Circum- 
feribéed SFigurés) ufed to fays AU excepe “the 

Greatef,-and’ AWexcept ‘the sing 9 ic Cae gai iT. 
Lin. cae 

Particular: Cafe 
dk «3 4 thle 48 be well’ known} edist? ets 
Terreftrial’ ¢) all ‘the Me dans’ theet ae 


MaifeelaneaCuriofa. = BX 


‘the Poles; (av EP. EP, Fig 3.) whereby the 


Parallels to the Equator , as they be nearer to 
the Pole, do continually ‘decreate. 
1p. And hereby a degree of Longitude in 


-fach Parallels, is lefs than a degree of Longi- 
tude in the: Equator, of a degree’ “of Latitude. 

12. And) that,:in. fuch proportion, as is the 
-€o-fine of Latitude (which is the femidiamiter 
-of fuch Parallel,) to the Radius of the Globe, 


or of the Equator. 
13./Yetchath it been thought fit (for fome 
reafons) to reprefent thefe Meridians, in the 


» Sea Gheire, by Parall eb ftraight lines 51as EP, 


ed 6 


TH, AMWhereby, es oe allel to the Poehter 
(as L A) was reprefented in the Sea-Chart, 
(as la,) as equal to the Equator £E: and.a 


degree of Longitude thereia, as lar ge as in the 


Equator. 
1geBy thisimeans, each dears: of Lanet- 


- tude in) fuch Parallels, was’ increafed, beyond 


+ 


its jaft proportion, at fuch rate as “the Equa- 
tor (or its Radius) is greater than fuch Paral- 


lel, Cor the Radius thereof.) 


16. But, in the Old Sea- Charts, the déevers 


of: Latitude were yet reprefented ‘(as they are 


in’ themfelves) ‘equal! to each other ; ‘and, to 


 thofe of the Equator. 


17. Hereby, amongft many other Inconve- 


-miencres, (as Mr. Edward Wright obferves, in. 


\ his: Correttion.of Errors in Navigation, firft pu- 


blifhed in the Year 1599,) the reprefentation 


“of Places remote froin the Equator, was fo di- 
' ftorted, in thofe Charts, as that (for inftance) 


an Tland i in the Latitude of 6o degrees, (where 


the Radius of the Parailel is but half fo great 
ee f oe of the Equator) would have its Length 


(frem 


‘42 «=Mifcellanea Curtofa, — 
(fromEaft to Weft)in comparifon of its Breadth 
(from North to South) reprefented in a dou- 
ble proportion of what indeed it is. , 

18. For rectifying this in fome meafure (and 

-of fome other inconveniences)Mr.Wright advi- 
feth ; that (the Meridians remaining Parallel, 

-as before) the degrees of Latitude,remote from 
the Equator, fhould at each Parallel, be pro- 
ah in like proportion with thofe of Longi- 
tude. : 

19. That is; As the Co-Sine of Latitude, 
(which is the Semi-diameter of the Parallel) 
to the Radius of the Globe, (which is that of 
the Equator: ) fo fhould be a degree of Lati- 

“tude, (which is every where equal to a degree 
of Longitude in the Equator,) to fuch a de- 
gree of Latitude fo protracted (at fuch diftance 

‘from the Equator;) and fo to be reprefented 
in the Chart. | 

20. That is, every where, in fuch proporti- - 
on asis the refpective Secant (for fuch Lati- — 
tude) to the Radius. For, as the Co-fine, to | 
the Radius; fo is the Radius to the Secant (of 

the fame Arch or Angle ;) as Fig. 4.2-R:: 

R 


- 21. Sothat ( by this means) the pofition of 
each Parallel in the Chart, fhould be at fuch © 
diftance from the Equator, compared with fo 
many Equinottial Degrees or Minutes, (as are 
thofe of Latitude,) as are all the Secants (ta- 
ken at equal diftancesin the Arch) to fo many 
times the Radius. nn 

22. Which is equivalent, (as Mr. Wright 
there notes) to the Projection of the Spherical 
furface (fuppofing the Ey-at theCenter)on the | 

concave furface of a Cylinder, erected at right 

' Angles to the Plain of the Equator. 
Hayek) : 24. And 


—Mifcellanea Curiofe: 12 
_ 23. And the divifion of Meridians, repre 
fented by the furface of a Cylinder ere&ted (on 
the Arch of Latitude) at right Angles, to the 
Plain of the Meridian (or a portion thereof.) 
The Altitude of fuch Projection, (or portion of 
- fuch Cylindrick furface) being (at each point 
of fuch Circular bafe) equal to the fecant (of 
Latitude) anfwering to fuch point. As Fig. §. 
. 24. This Projection (or portion of the Cy- 
lindrick furface) if expanded into a Plain, will 
be the fame with a Plain Figure, whofe bafe is 
equal toa Quadrantal Arch extended (or a 
‘portion thereof) on which (as ordinates) are 
erected Perpendiculars equal to the Secants, 
 anfwering to the refpedtive points of the Arch 
fo- extended: The leaft of which (anfwer- 
ing to the Equinoétval) is equal to the Radius; 
and the reft continually increafing, till (at the 
Pole) it be infinite. As at Fig. 6. 

25. So that, as ER/L. (a Figure of Secants 
erected at right Angles on EL, the Arch of 
- Latitude extended,) to ERRL, (a rectangle 

onthe fame bafe, who’s altitude ER is equal 
to the Radius; ) fo is E Z (an Archof the E- 
‘quator equal to that of Latitude,) to the di- 
fines of fuch Parallel, (in the Chart) from the 
Equator. 

26. For finding this diftance, anfwering to 
each degree and Minute of Latitude; Mr. 
Wright (as the moft obvious way) adds all the 
Secants (as they are found calculated in the > 
Trigonometrical Canon) from the beginning, 

! rae degree or Minute. of Latitude propo- 
fed. | ; 

- 29. The fum of all which, except the Great- 
eft, (anfwering to the Figure Infcribed) is too 

Little: ‘The fum of all except the Leaft, (an- 
ee ; | fwering 


14 Mifcellanea Curwfa- 
fwering to the Circumfcribed,) is too Great, 
(which i is that he follows : ) And it would be 
nearer to the Truth than either, if (omitting | 
all thefe) we.take the intermediates ;-for Min. 
ly fs 2% 335 @c. or (the doubles " of thefe) 
Min. 1,3, 5,7, ce. Which yet (becaufe on 
the Convex fide of the Curve) would be fome- 
what too Little. al 

28. But any of thefe ways are exact enough 
for the ufe intended, -as. creating No fenfible 
difference in the Chart. | 

29. If we would be more exad ; Mr. oie 
tred direéts (and fo had Mr. Wright done be- 
fore him) to divide the Arch into parts yet 
fmaller than Minutes, and. calculate Secaiits 


fuiting thereunto. ” 
30. Since the Arithmetick of infinite’ intto- 


- Pik b> 


without st come toa 7 dorechdnees propor- 
tion ;.) Methods have been found for {quaring 
fome fuch Figures ; and (particular lyCthe Ex- 
terior, Hyperbola (ia a way of continual ap- 
proach ) by the help, of an Infinite feries. . As, 
in the Philofophical Tranfaclions, Numb. 38, (for 
the Month of -Aaguff, 1668, ) And my. Book, 
De sie Cap. 5. Prop. 3r. | 

. In Imitation whereof, it hath been defi- 
at a find) by fome, t that a like Quadrature 
for this Figure of Secants (by an Infinite feries 
_ fitted thereunto) might be found. 
32. In order to which, put we for the Radi- 
us of a Circle, R ; the right Sine of an Arch 
or, Angle, S,, the Verfed Sine 5, V, the-Co-Sine 
(or Sine of the. Complement) ee pEaie eV SW: 
apa the Secant, i the Tangent, ‘T. Fig: 


ing 
. 33. Then 


Mifcelianea Curiofa. vf 
33. ‘Then i IS, . Se R: ER. W 9 That is, a R% 
pag ; the Secant, r ayitoed ? : oy 


eee ‘And 2S RT. That 52)SR TS 
the Tangent. 


prt Now, if we. fuppofe the Radius C P, Fe 


. divided into equal Parts, (and each of them, : 


ibs R;) and, on thefe, to be erected the Co-, 
Sines of Latitude LA: 
36. Then are the Sines of Latitude in Arithe, 
metick Progreffion. 


37° And the Secants anfwering thereunto,. 
| Lf=4 =" we 


38. But thefe Secants, (anfwering to right 
Sines in Arithmetical Progreflion) are not thofe, 
that ftand at equal diltance on the Quadran- 
tal Arch extended, Hig. 6. | 

39. But ftanding at unequal diftances (on 
the fame extended Arch; ) Namely, on thofe 
points thereof, whofe right Sines (whilft it was: 
a Curve) are in Arithmetical Progreilion. As, 
Fig. 8. 

40. ap! find therefore the magnitude of RE: 
Lf, Fig.6. Which is'the fame.with that’ of, 
Fig. 8. phate EL of the fame length in 
both; however the number of Secants therein 
may. be unequal: ) we are. to confider the Se-. 

cants, tho’ at unequal diftances: Fig. 8. to be: 
the fame with thofe at equal diftances in: Fig: 
7. anfwering to Sines in Arithmetical Progref- 
fion. 

4l. Now thefe Intervals, (or portions of the 
bafe) in Fig. 8. are the fame with the inter- 
iG cepted Arches (or ‘portions of the Arch) in Fig. 

_ -74'For this bafe is but tbat Arch extended. . 


A | 42, And 


5 z 
Saar a aS 


16 Mifcellanea Curiofa. 

42. And thefe Arches (in parts infinitely 
fmall) are to be reputed equivalent tothe por- 
tions of their refpective Tangents intercepted 
Between the fame ordinates. As in Fig.7- 9. 

43. That is, equivalent to the portions of 
the Tangents of Latitude. | 

44. And thefe portions of Tangents are, to 
the Equal intervals in the bafe, as the Tan- 
gent (of Latitude) to its Sine. 

45. To find therefore the true Magnitude of 
the Parallelograms (or fegments of the Figure; ) 
we muft either protract the equal fegments o 
the bafe, Fig. 7. (in fuch proportion as is the 
refpective Tangent to the Sine) to make theni 
equal to thofe of Fig. 8. : 

46. Or elfe (which is equivalent). retaining 
the equal intervals of Fig. 7. protract the Se- 


cants in the fame proportion. (For, eitherway 


the Intercepted Rectangles or Parallelograms 
will be equally encreafed) As L 1 Fig. 9. 

47. Namely; As the Sine (of Latiude) to 
its Tangent ; fo is the Secant to a Fourth; 


which is to ftand (on the Radius equally divi- 


| ded) inftead of that Secant. 


SR “Re R3 Spe ee 
S.S(::=-R):: | s7eReso=L M, Fig.o. 


48. Which therefore are as the Ordinates | 


. kn Qwhat I call Arith. Infin. Prop. 104) Recipro- 
ca Secundinorvum: fuppofing =? to be fquares 
in the order of Secundajies. 


— Mifecilanen Cnriofa. « 19 


2 3 5) ' 9 t : S» S$ 1 
Boe fits) RGR igstaeeth 
; 4] 4 a oe : ~ c R3-S2R. P 
49. This becauie oi aera 


| hy pata Japa S4. 
= *=RY-S',& the Sines +-S°R7R 
$, in Arithmetical Pro- 


greffion) is reduced (by) 4.54 
divifion) into this Iof- R a 
nite Series. | it ys 124 Wei! 
hy. ae aS 
R-- een Re &c ; : 


Yo. ‘That is(putting R=1.) hp; 
. Ll S*.\- S44. $°, &c. : , ) 


_ §1. Then.(according to.the Arithmetick of 
Infinites) we are to interpret S, fucceflively, by 

1 S, 2S, 3 S, &c. till we come to 5, the great- 
eft, Which therefore reprefents. the number 
of All. | 

52. And becaufe the firft Member.doth re- 
prefent a Series of Equals; the fecond of Se- 
Beats the third, of Quartans, @c. There- 
fore the firft Member is to be multiplied by S$; 
the fecond, by}S ; the third, by; 5; the 
Mourth, by 75; cc. 
~ 53. Which makes the Aggregate, 
— $tistt+is7+is’+,s’, &=ECLM, 


. becaufe S is always lefsthan R= | 
may be fo far continued, till fome power of 


tording to Mr. Wright’s defign: ) Having the 


y 


18 Mifcellanea Curiofa. 
propofed ParaJlel (of Latitude) given; we are’ 
to find (by the Trigonometrical Canon) the 
Sine of fuch Latitude, and take, equal to it, 
CL=s8. And, by this, find the magnitude of ~ 
ECLM, Fig. 9; thatis, of RELA Fig. 8. — 
that is, of REL, Fig.6. And then, as R 
RLE (or fo many times the Radius,) toR BE 
Lf (the Aggregate of all the Secants;) fo 
muft bea like Arch of the Equator (equal to 
the Latitude propofed,) to the diftance of 
fach Parallel, (reprefenting the Latitude in the 
Chart) from the Equator. Which is the thing 

required. | | 

56. The fame may be obtained, in like man- 

ner, by taking the Verfed Sines in Arithmeti- 
cal Progreflion. For if the right Sines (as here) 
beginning at the Equator, be in. -Arithmetical 
Progreffion, as 1, 2, 3, @c. Then will the Ver- 
fed. Sines, beginning at the Pole, (as being 
their complements to the Radius) be fo alfo. © 


The Collettion of Tanvents. 


57. The fame may be applied in like man- 
ner, (though that be not the prefent bufinefs,) 
to the Aggregate of Tangents, (anfwering to 
the Arch divided into equal parts.) = ; 

58. For, thofe anfwering to the Radius fo 


divided, are S~3 ( taking S. inArithmetical Pro- 
greffion.) Steyn SE ae 

_ §9- And then, inlarging the, Bafe, (Cas in 
Fig. 8.) or the Tangent (as in Fig.’9.) in the 


3 


proportion of the Tangent to the Sine. 


Plate J pageso 
: OS ae Bao 


Maifcellanea Curiofa. 19 


= Ne al SR2: SR2 
Ss. = ue ee OE oy Se R2--S2° 
60. e. have (by Divifion) this Serles, 
: : ins 
| R? S)SR? (S,+ So +gor 


R4 
Sigite S54 P78 Ba a ee 


pom 


61. That is(putting ee ue 4538 
Si. S3 Ss 97 1S, &ce 


62. Which (multiplying 3s 
thie refpective members by i oy e) 
| 3S, 495 = 9 ay: 1.95 &c.) be- he "Ra 


-comes | 
idle Se : 445% 4.651% &e, 4, $7 


Which is the onaalies of Tangents to the 
Arch, whofe right Sine is S. 

.. 63. And this method may be a pattern for | 
the like procefs in other cafes of like nature. 


3 


An 


20  Mifcellanea Curtofa. 


An eafte Demonflration of the Analo-— 
wy of the Lovarithmck Tangents 
to the Meridian Line or [um of tbe 
Secants ; with various Methods 
for computing the [ame to the utmoft 
Exacine|s,*oy E. Halley. | 


T is now near 100 Years fince our Worthy 
Countryman, Mr. Edward Wright, publith- 

ed his Correéttion of Errors in Navigation, a Book 
well deferving the perufal of all fuch as defign 
to ufe the Sea. Therein he confiders the Courfe 
ofa Ship on the Globe, ftearing obliquely to 
the Meridian ; and having fhewn, that the De- 
parture from the Meridian, is in all cafes lefs 
than the Difference of Longetude, in the rats of 
Radius to the -fecant of the Latitude, he con- 
cludes, That the fum of the Secants of each 
point of the Cuadrant being added fucceflively 
would exhibit a line divided into Spaces, fuch 
as the intervals of the parallels of Latitude 
ought to be ina trueSea-Chart,whereon theMe- 
-ridians are made parallel Lines, and the Rhombs 
or Oblique Courfes reprefented by right Lines. 
This is commonly known by the name of the 
Meridian Line,which tho’ it generally be called 
_Mercator’s, was yet undoubtedly Mr. Wright’s 
Invention, (as he has made it appear in his 

' Preface.) And the Table thereofis to be met 
with in moftBooks treating of Navigation,com- 
puted with fufficient exattnefs for the dae 
eA | C 


) ViifceHanea Curiofa. 21 
' * Te-was firft difcovered by Chance, and as far 
as licamdearn, firft publifYd by Mr. Henry 
Bond, as an addition to Norwood’s Epitome of 
Naviration, about 50 Years fince, that the A7- 
ridian Line was analogous to a Scale of Lozarith- 
mick, Tangents of half the Complements of the 
Latitudes. The difficulty to prove the truth 
of this Propofition, feemed fuch to Mr. Aer- 
_cator, the Author of Logarithmotechnia, that he 
propofed to wager a good fum of Mony,againit 
whofo would fairly undertake it, that he fhould 
not demonftrate either, that it was true of 
falfe: And about that time Mr. fobx Collins, 
holding a Correfpondence with all the Eminent 
‘Mathematicians of the Age, did excite them 
tothis enquiry = = 
* The firft that demonftrated the faid Azalogy, 
was the excellent Mr. Fames Gregory in bis Ex- 
ercitationes Geometrice, publifhed Anno 16658. 
which he did, not without a long train of Con- 
fequences and. Complication of Proportions, 
whereby the evidence of the Demonftration is 
in a great meafure loft, and the Reader wea- 
ried before he attain it. Nor with lefs work 
and apparatus hath the celebrated Dr. Barrow, 
in his Geometrical Leétures (Lect. XI. App. 1.) 
proved, that the Swm of all the Secants of 
any arch is analogous tothe Logarithm of the 
ratio of Radius -\- Sine to Rad.—Sine, or, which 
is all one, that the Meridional parts anfwering 
to any degree of Latitude, are as the Logarithms 
of the rationes of the Verfed Sines of the diftan- 
ces from both the Poles. Since which the in- 
comparable Dr. Wallis (on occafion of a Para- 
logifm committed by one Mr. Zvorris in this 
matter) has more fully and clearly handled this 
Argument, as may be feen in Num. 176. of 
Ry tid 3 the 


22 Maifcellanea Curiofa. q 
the Tranfattions. But’ neither Dr. Wallisnor 
Dr. Barrow, in their faid Treatifes, have any 
where touched upon the aforefaid relation of 
the Meridian-line to the Logarithmick Tangent ; 
nor hath any one, that 1 know of, yet difcover- 
ed the Rule for computing independently the 
interval of the Aeridional parts anfwering, to’ 
any two given Latitudes. a 

Wherefore having attained, as I conceive, a 
very facile and natural demonftration of the 
faid Analogy, and having found out the Rule 
for exhibiting the gifference of Meredional parts, 
between any two parallels of Latitude, without 
finding both the Numbers whereof they are the 
difference: I hope I may be entituled to a 
fhare in the Improvements of this ufeful part 
of Geometry. And firft, let us demonftrate 

the following Propofrtion. 6 otenart bor 

The Meridian Line is a Scale of Logarithmick, 
Tangents of the half Complements of the Latitudes. . 

For this Demonftration, it is requifite to 
premife thefe four Lemmata. 


Lemma. \. In the Stereographick, Projettion of 
the Sphere upon the plain of the Equinodiual, 
the diftances from the Center, which in this — 
cafe is the Pole, are laid down by the Tan- 
gents of half thofe diftances, that is, of half 
the Complements of the Latitudes. This is 
evident from Eucl. 3. 20. | 


Lem. Vi. In the Stereographick Projection, the 
Angles under which the Circles interfect each 
- other, are in all cafes equal to the Spherical. 
Angles they reprefent: Which is perhaps as 
valuable a property of this Projeétion, as that 
of all the Circles of the Sphere thereon appear-. 

| ee 


Maifcellanea Curtofa. 22 
“ing Gircles: But this not being vulgarly known, 
-muft not be aflumed without a Demonjftration. 
Let EBPL in Fig. 1. Tab. 2. be any great 
circle of the Sphere, Ethe Eye placed in Its 
Circumference, C its Center, P any point 
thereof, and let FC O be fuppofed a plain 
erected at right Angles to the Circle E BP L, 
on which FCO we defign the Sphere to be 
projected. Draw E P crofling the Plain F 
CO inp, and p fhall be the Point P projected. 
To the point P draw the Tangent A P G 
and on any point thereof, as A, erect a per- 
pendicular AD, at right angles to the plane 
EBPL, and draw the lines PD, AC, DC: 
and the AngleAPD fhall be equal to the Sphe- 
_rical Angle contained between the plains 4 P 
C, DPC. Draw alfo AE, DE, interfe&ing 
the plain FC9 in the points 2 and d; and 
joyn ad, pd: I fay the Triangle 2d is fimu- 
‘Jar to the triangle 4DP. And the Angle apd 
equal to the Augle APD. Draw PL, AK, pa- 
rallel to FO, and by reafon of the parallels, 4 
pwill be toad as AKto AD: But (by Excl. 
3. 32.) in the triangle AKP, the angle AKP= 
LPE is alfo equal to APK= EPG, wherefore 
the fides AK, AP, are equal, and ’twill be as 
aptoad fo AP to AD. Whence the angles 
DAP, dap being right, the angle APD will 
be equal to the angle zpd, that is, the Sphe- 
rical Angle is equal to that on the Projection, 
and that in all Cafes. Which was to be proved. 
This Lemma | lately received from Mr. 46. 
de Moivre, though! fince underftand from Dr. 
Hook, that he long ago produced the fame 
thing before the Society. However the demon- 
{tration and the reft of the Difcourfe, is my 
own. 
C4 Lemma 


24 Maifcellanea Curiofa. i! 


Lemma Il. On the Globe, the Rumb Lines 
make equal angles with every Meridian, and — 
by the aforegoing Lemma, they muft like-_ 
wife make equal angles with the Meridians in 
the Stereographick Projection on the plain of the - 
Equator; They are therefore,in that Projection, 
Proportional Spirals about the Pole Point. . 


Lem JV. in theProportional Spiral (Fig.2.)it is 
a known property,that the angles BPC, or the. 
arches BD, are E.cponent's of the rationes of BP 
to PC: for if the arch BD be divided into in- 
numerable equal parts, right lines drawn from 
them to the Center P, fhall divide. the Curve B 
ccC, into an infinity of proportionals ; and all 
the lines Pe fhall be an infinity of proportionals 
between PB and PC, whofe number 1s equal to 
all the points d,d, in the arch BD: Whence 
and by what I have deliver’d in the next enfu- 
ing Difcourfe it follows, that as BD to Bd, or 
as the angle BPC to the angle BPc, fois the 
‘Logarithm of the ratio of PB to PC, to the Lo- 
garithm of the ratio of PBto Pc. 
. From thefe Levmata our Propofition is very 
clearly demonftrated :. For by’the firft, PB, 
Pc, PC are the Tangents of half the Comple- 
ments of the Latitudes in the  Stereographick, 
Projeétion: and by the laft of them, the diffe- 
rences of Longitude, or angles at the Pole be- 
tween them, are Logarithms of the ratzones of 
thofe Taugents one to the other. “But the Nau- 
tical Meridian Line, is no other than a Table 
of the Longitudes, anfwering to each minute 
of Latitude, on the Rhumb-line, making an 
angle of 45 degrees with the Meridian Where-_ 
fore the Meridian Line is no other than a Scale 
of Logarithmick Tangents of the half aeats 
) ments 


% 


Mifcellanea Curiofa. aaa. 


_ ments ofthe Latitudes. Quod erat demonftran- 


dum. 

Coroll. 1.Becaufe that in every point of any 
Rhum Line, the difference of Latitude is to the 
Departure, as the Radius to the Tangent of the 
angle that Rhumb makes makes with the Me- 
ridian; and thofe equal Departures are every 
where to the differences of Longitude, as the 
Radius to the Secant of the Latitude ; it fol- 


ows, that the differences of Longitude are, on 
_any Rhumb, Logarithms of the fame Tangents, 


but of a differing Species, being proportioned 
to one another as are the Tangents of the ai- 
gles made with the Meridian. 

Coroll, 2. Henceany Scale of Logarithm Tan- 
gents, (as thofe of the Vulgar Tables made 
after Bricgs’s form; or thofe made to Nzapier’s, 
or any other form whatfoever) is a Table of 
the differences of Longitude, to the fevera] La- 
titudes, upon fome determinate Rhumb or o- 
ther: And therefore, as the Tangent of the 
angle of fuch Rbhumb, to pe Tangent of any 
other Rhumb: So the difference of the Loga- 
rithms of any two Tangents, to the difference ° 


of Longitude, on the propofed  Rhumb, inter- 


cepted between the two Latitudes, of whofe - 
half Complements you took. the Logarithm 
Tangents. . 

And fince we have a very compleat Table 
of Logarithm Tangents of Briggs’s form, publish- 
ed by Vlacq, Anno 1633, in his Canon Magnus 
Triangulorum Logarithmicus, computed to ten 
Decimal places of the Logarithm, and to every 
ten Seconds of the Quadrant (which feems to 
be more than fufficient for the niceft Calcula- 
tor) I thought fic to enquire the Oblique angle, 
with which that Rhumb Line crofles the or 

ridian, 


26 Maifcelanea Curiofa. 

ridian, whereon the faid Canon of Valcg: pre- 
cifely anfwers to the differences of Longitude, 
putting Unity for one minute thereof, as in 
the Common Meridian Line. Now;-the mo- 
mentary augment or fluxion of the Tangent Line 


at 45 degrees, is exactly double to the fluxion 


of the arch of the Circle, (as may eafily be 
proved) and the Tangent of 45 being equal to 
Radius, the fluxion alfo of the Logarithm Tan- 
gent will be double to that of the arch, if the 
Logarithm be of Napier’s form : but for Briggs’s 
form, it will be as the fame doubled arch, mul- 
tiplied into 0, 43429, &c. or divided by 2, 
30258, &c. Yet this muft be underftood only 
of the addition ofan indivifible arch,for it cea- 
fes to be true, if the arth have any determi- 
nate magnitude. ye | | 
Hence it appears, that if one minute be fup- 
pofed Unity, the length of the arch ofone mi- 
nute being ,00029088820866 5721596154, KC. 
in parts of the Radius, the proportion will be 
as’ Unity to 2,908882, &c. fo Radius to the 
Tangent of 71° 1/ 42'? whofe Logarithm is 10. 
4637261172071832§204, &c. and under that 
angle is the Meridian interfected by that 


Rhumb Line,on which the differences of Napier’s 


Logarithm Tangents of the half Complements 
of the Latitudes are the true differences of Lon- 
citude, eftimated in minutes and parts, taking 


the firft Four Figures for Integers. But for- 


Vlacq’s Tables, we muft fay. . | 

As .2302585, &c. to 2908882, &c. So Ra- 
dius to 1,26331143874244569212, &c. which 
is the Tangent of 51° 38 9”, and its Logarithm 
10,101 §10428507720941162, &c. wherefore in 
the Rhumb Line, which makes an angle of 51° 
33’ 9” with the Meridian, Vlacq’s Logarithm 


Tan- 


= Ge 


Mifcellanea Currofa. ey: 
Tangents are the true differences of Lon- 
gitude. And this compared with our fecond 
Corollary may fuffice for the ufe of the Tables 
already computed. : 

_ But if a Table of Logarithm Tangents be 
made by extraction of the root of the Infiniteth 
power, whofe Index is the length of the arch 
- you put for Unity, (as for minutes the ,ooo 
—-2908882th,&c. power) which we will call a; 

fuch a Scale of Tangents fhall be the true Me- 
ridian Line, or fum of all the Secants taken 
infinitely many. Here the Reader is defired 
to have recourfe to my little Treatife of 
Logarithms, in the enfuing Difcourfe that I 
may not need to repeat it. By what is there 
delivered,it will follow, that putting ¢ for the 
excefs or defect of any Tangent above or under | 
the Radius or Tangent of 453; the Logarithm 
of the ratio of. Radius to fiuch Tangent will be 

é into ¢—tee |. $ete— freee + +t5,&c. 
when the arch is greater than 45 5" OF 
Pe intoe + 4ee-+ 323 40+ + 405, &e. 

when it is lefS than 45¢r. And by the fame do- 
rine putting T for the Tangent of any arch, 
and ¢ for the difference thereof from the Tan- 


gent ofanother arch, the Logarithm of their 
yatio will be 
hints ie ne eee Stn 
minto rb orp 575 Vie 
when T is the greater Term, or 


i if tt 4a Peta, Be $ 
into > — ary} ant as Gr, &e 


hen T is the lefler Term: - LLasies 
he And if.m be fuppofed 0002908882, &e. = 


the 


23 Maifcellanea Curwfa. 

: r : 
a, its reciprocal > will be, 3437574977973493 
92326, &c. which multiplied into the afore+ 
faid Series, fhall give precifely the difference of 
Meridional parts, between the two Latitudes, 
to whofe half complements the aflimed Tan- 
gents belong. Nor is it material from whe- 
ther Pole you eftimate the Complements,whe- 
ther the clevated or deprefled , the Tangents 
being to one another in the fame ratio as their 
Complements, but inverted. rate 

In the fame Difcourfe I alfo fhewed, that 
the Series might be made to converge twice as 
fwift, allthe even powers being omitted sand 
putting 7 for the fum of the two Tangents, the 
fame Logarithm would be 


$y st 
je -|- ts 


7 Ree suas ti a gag 
"A Or 1 into a 373 erry 979 te 


oe 
but the ratio of 7 tot, or of the fum of two 
Tangents to their difference, is the fame as 
that of the fime of the fum of the arches, to the 
fine of their difference. Wherefore, if S be put 
for the fie Complement of the Middle Lati- 
tude, and s for the fine of half the difference 
of Latitudes, the fame Serves willbe 


ar. is sige a ee : 


iad 


wherein, as the differencts of Latitude are 
fmaller, fewer fteps will fuffice. And if the 
Equator be put for the middle Latitude, and 
confequently S==R, and s to the five of the La- 
titude, the Meridional parts reckoned from 
the Equator will be | Ot as Vibha 


§ 
& 


_ 


Mifcellanea Curiofa. 29 


x 
a : 
—— &c. 


sf | S iH sf 
Te 3 Pe ie | 3 : 
a 317 & 57 @ Sd ar 


which is coincident with Dr. Wallzs’s folution 
in Numb. 176. of the Philofophical Tranfattions. 
And this fame Series being half the Logarithm 
of the ratio of R-+-s to R—-s, that is, of the Ver- 
_fed-fines of the diftances from both Poles, does 
agree with what Dr. Barrow had fhewn in his 
Xith. Ledture. a : 
“The fame ratio of > tot may be expreffed alfo 
by that of the Swm of the Co-fines of the two Lati- 
tudes, to the fine of their difference: As likewife 
by that of the Sine of the Sum of the two Lati- 
tudes, to the difference of their Co-fives: Or by 
that of the Verfed-fine of the Sum of the Co-lati- 
tudes, tothe difference of the fines of the Latitudes: 
Or as the fame difference of the fines of the Latte 
tudes, to the Verfed-fine of the difference of the La- 
titudes . all which are in the fame ratio of the 
Go-fine of the middle Latitude, to the Sine of 
half the difference of the Latitudes. As it 
were eafie to demonftrate, if the Reader were 
not fuppofed capable to do it himfelf, upon a 
_ bare infpection of a Scheme duly reprefenting 
thefe Lines: 3 Le 
This variety of Expreflion of the fame ra- 
tio {thought not fit to be omitted, becaufe by 
help of the rationality of the Sine of 3097. 
in all cafes where the Sum or difference of the 
Latitudes is 3097. 6ogr. gogr. 120¢r. or 1§0 
degrees, fome one of them will exhibit a fimple 
feries, wherein great part of the Labour will be 
faved : And-befides 1 am willing to give the 
‘Reader his choice which of thefe equippolent 
methods to make ufe of ;-but for his exercife 
of | fhall 


20 M t{[cellanea Curiofa. 


fhall leave the profecution of them, and the 


compendia arifing therefrom,to his own Induftry. 
Contenting my felf to confider only theformer, 
which for all ufes feems the moft convenient, 
whether we defign to make the whole Meri- 
dian Line, or any part thereof, viz. : 


¥ S us $ 
oY BA § s 5 pest § S 
— into =-+ —=- —— + 

a 


EY ar iter Ae rggs eG 


Wherein @ is the length of any Arch which 


you defign fhall be the Integer or Unity in 


your Meridional Parts,(whether it bea Minute, 
League, or Degree, or any other,) S the Co- 


fine of the Middle Latitude, and s the Sine of - 


half the difference of Latitudes; but the Se- 
cants being the Reciprocals of the Co-fines, 


= will be equal to putting {for the Secant 


of the Middle Latitude; and — into = will 
caer Ae multiplied by 355 that is by 
ffss 


3777s 


will give the fecond ftep: and that a- 


gain by A the third ftep ; and fo forward, 


till you have compleated as many places as you 
defire. But the fquares of the Szves being in 
the fame ratio with the Verfed-fines of the dou- 


ble Arches, we may inftead of szyallume for 


our Multiplicator est or the Verfed-fine of 


3K 


4 


the 


_ ; aren eee de elle 
eto. lL pap ictal bw le aca i i al i atl 


Mifcellanea Curiofa. 31 


the difference of the Latitudes,divided by thrice 

the Verfed-fine of the fum of the Co-latitudes, 
&c. which is the utmoft Compendium | can think 
of fer this purpofe, and the fame /eries will 
become, ms . 


ee et LP pe ve Ue oe 
i as BR SV AT Fh ipe 


Hereby we are enabled to eftimate the de- 
fault of the method of making the Meridian 
line, by the continued addition of the Secants 
of equidifferent Arches, which as the difference 
of thofe Arehes are finaller, does ftill nearer | 
and nearer approach the Truth. Ifweaffume, 
as Mr. Wright did, the Arch of one minute to 
be Unity, and one minute to be the common 
difference of a rank of Arches: It will be in all 
cafes, as the Arch of one Minute, to its Chord 
:: So the Secant of the middle Latitude, to 
the firft ftep of our feries. This by reafon of 
the near equality between 2 and 25, which are 
to one another in the ratio of Unity to 1—0, 
- ©000000035§2566457713, &c. will not differ 

_ from the Secant fbut in the ninth Figure; be- 
ing lefs than it in that proportion. The next 


oe 3 3 és 
ftep being st 2s will be equal to the Cube | 
of the Secant of the middle Latitude multipli_ 


ie eee 


Ae 555° 
ed into ar 0,000000007051 32908715 ; 


which therefore unlefs the Secant excéed ten 
_ times Radius, can never amount to 1 in the fifth 
place. Thefe two fteps fufhce to make the 
Meridian Line, or Logarithm Tangent to far 
more’places than any Tables of Natural Se- 
; cafes, 


EM OT er ten 


22. M ife ni C fa 


cants yet extant, are computed to; butifthe — 
third ftep be required, it willbe found tobe 


DAC 
4-5 into eae 0000000000000000894598 5 


By all which it appears, that Mr. Wricht’s 
Table does no where exceed the true Meridian 
Parts by fully half a Minute: which finall dif- 
ference arifes by ES having added continu ually 
: the Secants of 1’, 2’, 3’, &c. inftead of 037,12, 
2/55 32, &c, But asit is, it is abundantly fuf-— 
ficient for Nautical Vfes. hatin Sir Jonas Afoor’s 
New Syftem of the Afathematicks, is much near- 
-erthe Truth, but the difference from Wright 

is fcarce fenfible till you exceed thofe Latitudes 
where Navigation ceafes to be practicable, the 
one exceeding the Truth by about half a Mi- 
nute, the other being a very fmall matter de- 
ficient therefrom. 

For an Example eafie to be imitated by who- 
fo pleafes, I have added the true Meridional 
Parts to the firft-and laft Minutes of the Qua- 
drant; not fo much that there is any occafion 
for fach occurrancy, as to fhew that | have ob- 
tained, and laid down herein, the-full Doctrine 
of thefe Spiral Rhumbs, which are of fo great 
concern inthe Art of Navigation.  - : 


‘7bne firft Minute is, I 60000001 41036$862178 
The Second, §'+.. ©2,00000005541063806707 
The Lait or 89° 59 is 30374963431 1414228643 


a not 32348, 5279 as Mr. Wright has it, by 
adding the Secants of every whole Minute: Nor. 
30249,8 as. Mr. Oughtred’s-Rule makes it, by 
adding the Secants: of. every other half Minute. 
-Not 30364,3 as Sir. Fonas Algor’ had concluded | 
. it 


— Mifcelanea Cutiofa. 22 
it by I know not what Method, tho’ in the reft 
of his Table he follows Oughtred. 

_ And this may faffice to fhew how to derive 
the true Meridian Line from the Sines, Tan- 
gents, or Secants fuppofed ready made ; but 
we are not deftitute of a Method for deducin 
‘the fame independently, from the Arch it felt. 
If the Latitude from the Equator be eftimated 
by the length of its Arch 4, Radius being U- 
nity, and the Arch put for an Jnteger be 4, as 
before; the Meridional parts anfwering to that 
Latitude, will be . 


—intodl3 4 4-34! jase 


e4 F\. +e. 
7 Aor 5045 4 k 2yie 
fA” or aii i Wn. 
P jal 


which converges'much: fwifter than any of the 
former Series, and befides has the advantage of 
A encreafing in Arithmetical progreflion,which 
would be of great eafe, if any fhould undertake 
de novo to make the Logarithm Tangents, or the 
Meridian Line to many more places than now 
we have them. The Logarithm Tangent to | 
the Arch of 45 - 3 A being no other than the 
aforefaid Series 4 +4 4? |, A’, &c. in 
“Napeir’s form, or the fame multiplied into 
0,43429, &c. for Brigg’s. | 

_ But becaufe all thefe Serzes toward the latter 
€nd of the Quadrant do converge exceeding 
flowly, fo as to render this Method almoft ufe- 
Tefs, or at leaft very tedious: It will be con- 
venient to apply fome other Arts, by afluming 
the Secants of fome intermediate Latitudes ; 
“and you may for s or the Sine of #2 the Arch of 
shalfthe difference of Latitudes, fubftitute -— 
ge Tate OM ayes 2 rater &c. accord- 


iy ing 


pea tat a fe hash Se ab i 
ea Chea i ees a ol, 


ee 

34  Mifcellanea Curiofa. 

ing to Mr. Newton's Rule for giving the Sine 
from the Arch: And ifabe no more than a 
Degree, a very few fteps will fuffice for all the 
_ accuracy that canbedefired. 

_ And ife be commenfurable to a, that is, if 
it be a certain number of thofe Arches with 


which you make your é#teger, then will £ be 
tate 

that number: which if we call 2, tbe parts. of’ 

the Meridional Line will be found to be, | 


(t -|- faa frat es fae, &e. 
‘r+ nF 7 rt= 
maa fat mm fies, &e 


fi. Sr. Gir 6 7.1? 
, inte 4 ge 5. 1i3fzas%, Ke. 
3 | 12074 J \(960)7* 3} 
woe The eg Ate 
; 5040 re 
L 


Inthis,the firft two fteps are generally fufhei- 
ent for Nautical ufes,efpecially when neither of 
the Latitudes exceed 60 degrees, and the dif- 
ference of Latitudes doth not pafs 30 degrees, 

But I am fenfible I have already faid too 
much for the Learned, tho’ too little for the 
‘Learner ; to fuch 1 can recommend no better 
-Treatife, than Dr. Wallies precedent Dif 
‘courfe, wherein he has with his ufual brevity, 
-and that perfpecuity peculiar to himfelf, hand- 
led this Subje& from the firft Principles, which 
here for the moft part we fuppofe known, _ 

I need not fhew how, by regreflive work, to 
-find the Latitudes from the Meridional Parts. 
the Method being fufficiently obvious. 1 shall 

-only conclude with the propofal of a aberen 
whic 


mn 


ew 


Mifeellanea Curtofa. 25 
which remains to make this’Doctrine compleat, 
and that is this. - 102 2% f 
_ A Ship fails from a given Latitude, and ha- 
ving run’a certain number of Leagues, has al- 
terd her Longitude by'a givemangle, itis re- 
quired to find the Courfe fteared. Thefolu- 
tion hereof would be very acceptable, if not 
to the Publick, at- leaft to the Author. of this 
Tratt, being likely to open fome further Light 
into the Myfteries of Geometry. © 

To conclude, I fhall-only addy That Uni- | 
ty being Radius, the Co-five of the Arch 4, 
according to the fame Rules of Mr. Nemtor, 
will be ‘ 


_ 


. 


to-b A 3 A ngs A bistas A ngs ais3 Ah KO 
from which and the former Series exhibiting 
the Size by the Arch, by divifion, it is. eafie 
to conclude, that the Natural Tanzent of the 
Arch 4,is ae 
An At Ot Aah 4, &e. 
and the Natural Secant to the fame Arch | 
ES As At AST A", &e. 
and from the Arithmetick of Infinites, the 
Number of thefe Secants being the Arch A, 


it follows, that the fum Total of all the In- 
finite Secants on that Arch, is 


| AT; wire vets Ai+yiite Dige XC 


Ch > he 
a . 
= Saat 4 : the 


36 Mifcellanea Curtofa. 
the which, by what foregoes, is the Logarithm 
Tangent of Napeir’s form, for the Arch of 4sgr. 
4-1 4, as before. | a 
' And Colle@ing the Infinite Sum of all the 
Watural Tangents on the faid Arch A, there 
williarlid  .£91597] 9 y aks : i 


pAAt A AME A baits AM its A, Ke. 
which will be found to be the Logaritm of the 
Secant ofthe fame Arch. 


: MifceHanea Curiofa. 27 


A moft compendious and facile Me- 
- thod for Conftrucing the Loga- 
_ rithms exemplified and demonftra- 
- ted fromthe Nature of Numbers, 
_ without any regard to the Hyper- 
bola, with a [peedy Method for 
finding the Number from the Lo- 
. garithm given. By E. Halley. 


“4H & Invention of the Logarithms is juft- 
“i ly efteemed one of the moft, Ufeful Dif- 
‘coveries in the Art of Numbers, and accord- 
ingly has had an Univerfal Reception'‘and Ap- 
plaufe; and the great Geometricians of this 
Age, have not been wanting to cultivate this 
Subje& with all the’ Accuracy and Subtilty a 
‘matter of that confequence doth require ; and 
‘they have demonftrated feveral very admira- 
ble Properties of thefe Artificial Numbers, 
‘which have ‘réndred their Conftruétion much 
-more facile than by thofe opetofe Methods at 
‘firft ufed by thelr truly Noble Inventor, the 
Bet any and our worthy Country-man 

TRAE Brey p9. 2! © A8% otto oda to radians.) oy 
Bat notwithftanding all their Bedeavours, I 
“find very fewf thofe: who) make conftant ufe 
of Logarithms,’ to: have attained an adequate 
Notion ofthem to know how ito make or ex- 
amine them 3! 6t-:to- cag thenextent if 
3 the 


38 Mifcellanea Curifa. 
ufe of them: Contenting themfelves with the © 
Tables of them as they find them, without da- 
ring to queftion them, or caring to know how — 
to réCifie. them, fhould they be found amifs; — 
being I fuppofe under the apprehenfion of fome — 
creat difficulty therein. +: For.the fake. of fuch 
the following Tra is principally intended,but — 
not without hopes however to produce fome- 
thing that may be acceptableto the moft know- 
payee Gel thefe \mattersissreyy wae Ay ae 
But firft,it maybe requifite.to premife a de- 
finition.of Logarithms, in order to render the 
enfuing Difcourfe more clear, the rather be- 
caufe the old one Numerorum proportionalium 
aqui differentes comites, feems too {canty to de- — 
fine them fally. They may more properly be 
faid to be Numer: Rationum Exponentes: Where- 
in we confider ratio as a Quantitas fui. generis, 
beginning ‘from the ‘ratio, of requality, or 1 to 
1==0; being, Affirmative when the ratio 1s 1n- 
-‘ereafing, as of Unity toa greater Number, 
’ “but Negative when -decreafing; and,thefe ra- 
tiones we fappofe to be meafured by the Num- 
“ber of ratiuncule contained) in each. Now.thefe 
-yatiuncula are fo to’be underftood as ina 
-continued Scale of Proportionals. infinite -in 
‘Number between the two terms of the ratio, 
* which infinite Number ofymean Proportionals 
‘is to that infinite Number of siete and equal 
“yatiuncule betweenvany other two. terms, as 
the Logarithm of the one ratio is tothe Loga- 
 sithm of the other. ‘Thus, if there be fuppo- 
* fed’ hetween 1and to an infinite Scale of mean 
© Proportionals, whofe Number is, 1©0000, Cc. 
~ Gn infinitum 5 between 1 and 2-there -fhall be 
30102, -C*c.. of fuch Proportionals,and between 
be e tt rast: “f 


Mifcelanea Curiofa. 39 


1 and 3 there will be 47712 Gc. of them? 
which Numbers therefore are the Logarithm’ 
of the rationes of 1 to 10, 1 to 2, and 1 to 3: 
and not fo properly to be called the Logarithms 

of 10, 2 and 3. : 

_ But if inftead of fuppofing the Logarithms 
compofed of a number of equal Ratiuycula, 

proportional to each ratio, we fhall 1 take 

the ratio of Unity to any number to confift 

always of the fame infinite number of Xa- 

tiuncula, their magnitude, in this cafe, wil! 

be as their number in the former; wherefore 

if between Unity and any Number propofed, 

there be taken any infinity of mean Proportio- 

nals, the infinitely little augment ‘or decre- 

ment of the firft of thofe means from Unity, 

will be a ratiuucula, that is, the momentum or 

Fluxion of the ratio of Unity to the faid Num- 

ber: And feeing that in thefe continual Pro- 

portionals all theratiuncule are equal,their Sum, 

or the whole ratzo will be as the faid momentum 

is directly ; that is, the Logarithm of each 

yatio will be as the Fluxion thereof. Where- 

fore if the Root of any infinite Power be ex- 

tracted out of any Number, the differentrola of 
the faid Root from Unity, fhall beas the Loga- 

rithm of that Number. So that. Logarithms 

thus produced may be of as many forms as you 

pleafe to affume infinite Izdices of the Power 

whofe Root you feek: as if the Index be fuppo- 

‘fed 100000@c. infinitely, the Roots fhall be the 

‘Logarithms invented by the Lord Napeir 5, but 

af the faid Index were 2302585, @c.Mr.Briggs’s 

‘Logarithms would immediately be produced. 

And if you pleafe to ftop at any number of 
Figures, and not to continue them on, it will 

Cs es ama Ta See Soe 


40 Muifcellanea Curiofa. 
fuffice to affume an- Index of a Figure or two 
more than your intended Logarithm is to have, — 
as Mr. Briggs did, who to have his Logarithms — 
true to 14 places, by continual extraGtion of 
the Square Root, at laft came to have the Root 
of the 140737488355328rh Power; but how 
operofe that ExtraGtion was,will be eafily judg-— 
ed by whofo fhall undertake to examine his 
— Calculus. ie 
Now, though the Notion of an Infinite Pow- 
er may feem very ftrange, and to thofe that 
know the difficulty of the Extraction of the 
Roots of High Powers, perhaps impracticable ; 
yet by the help of that admirable Invention of 
Mr. Newton, whereby he determines the Uncie 
or Numbers prefix’d to the Members compo- 
fing Powers ‘(on which chiefly depends the Do- 
étrine of Series) the Infinity of the Index con- 
tributes to. render the Expreffion much more 
eafie: For if the Infinite Power to be refol- 
ved be put (after Mr. Newron’s Method ) 


I * TEMS aa f pe at 
Pipa Pepg lm 8 Tam inftead of Ind Fr 
in |) amebomm , | 1—6m-\1 rmm—6m3 © 
2mm qq Tse ee 240k. g 
&c. (which isthe Root when is finité)becomes 
gh le ee 
oh ee Ooo sp Tamme Be maaan: Sith 
mm being imfimte infinite, and confequently 
whatever is divided thereby vanifhing. Hence 
it follows that ae multiplied. into 9-2 994-3 
gqq—. 4+ 49° &c. is the augment of the firft 
of our mean Proportionals between Unity and 
1+}-q, and is therefore the Logarithm of the 
ratio of 1 to 1-+q; and whereas the Infinite bie 


Yr 


— Mifcellanea Curiofa. 41 


dex m may be taken at pleafure, the feveral 
Scales of Logarithms to fuch Jzdices will be as 


—or reciprocally as the Indices. And if the 


idee be: taken 10000, &c. asin the cafe of 
Napeir’s Logarithms, they will be dimply ie. 
9903 999--; F151 29° &e 

Again, if the Logarithm of a Secteatiie raq- 
tio be “pagel the infinite Root of Iq or 


3 i" 


pe =7% &c. whence the. decrement of the 
fir ft oe infinite Number of Propor ian 
will be = into ght agjigitigt+igttig® 
which therefore will be.as the shing ’ 
the ratio of Unity tor—g. But if m be put 
"19000, &c: then the faid Logarithm will be 
qiaqtig igi ts 9° Taq’, &c. 
_. _ Hence the ferns of any ratio, heing 4 and é b, 


“gq becomes ~ - or the difference divided by 


the. leffer term, when ’ tis an increafing _ ratio; 
or, h @ when ’tis decreafi ing, or as b to 4. 


“Whence the Logarithm. of the fame ratio may 
_be doubly expreit, for putting ~ for the diffe- 
jade of the ter ms 4 and. b, it will be either. 


eas peat 


x2 x3 xt xs 36 
aa, OA Ly eae ae CXC. 


240 3 43 ree abs as 
But 


rai into = — 


A? Mifcellanea Curiofa. 


But if the ratio of ato b be fuppofed divi- 
ded into two parts, viz. into the ratio of 2 to_ 


the Arithmetical Mean between the terms, 
and the ratio of the faid Arithmetical Mean 
to the other term 6, then will the Sum of the 
Logarithms of thofetwo ratioves be the Loga- 
rithm of the ratio of a to. 6; and fubftituting 
+zinftead of }4‘+3 6 the faid Arithmetical 
Mean, the Logarithms of thofe ratzones will be 
by the foregoing Rule, | 


© ews OG we CS Fe x5 


= —s 


ea) eee etree 
® in oe ene eee —-——-— ‘Sr and me 
wm errrarr area lrcar sr: re | 


SES ge) gee Sigg a) aeB i Deg ST nat gee 
YQ ee | & 

ip tk Sh re avila 6.2% Cae 
the Sum!._ 2x 2x3 2x5 Ox? As 


. bethe Logarithm of the ratio of 4 to b, whofe 

‘difference is x and Sumz. And this ‘Series 
converges twice as fwift as the former, and 
therefore 1s more proper for the Practice of 
making Logarithms: Which it performs with 
that expedition, that where» the difference 
is but the hundredth part of the Sum, the 


firft ftep == fuffices to feven places of the 
Logarithm, and the fecond ftep to twelve: 


But if Briggs’s firft Twenty Chiliads of Loga- 
‘rithms be fuppofed made, as he has very care- 
fully computed them to fourteen places, the 
firft ftep alone, is capable to give the Loga- 
rithm of any intermediate Number true; to. all 
the places of thofe Tables. : 


After the fame manner may the difference 


of the-faid two Eogarithms be very fitly ap- 
: | bapa 


, 


Maifeellanea Curtofa. . An 
plied to.find the. Logarithms of Prime Num- 
bers, having the Logarithms of the two next 
Numbers above and below them: For the dif- 
ference of the ratio of ato + z and of yz tob 
is, the ratio of 2.6 to} xz, and the half of that 
ratio, is that of Vabto ! z, or of the Geo- 
metrical Mean to the Arithmetical. And 
confequently the Logarithm thereof will be the 
half difference of the Logarithms of thofe-rati- 
ONES, Vie!» eid 


Ge CONS ae ‘ 
x4 pia i, by 
— into — + — te AE 2 
2h 4rt } 62° 8z8 


Which is a Theorem of good difpatch to find 


_ the-Logarithm of 3 z. But the fame is yet much 


more advantageoufly performed by a Rule de- 
rived from the foregoing, and. beyond which, | 
in-my-Opinion, nothing better.can be hoped. 
For the ratio of abtoz zzor', aattab+% 
bb, has the difference of its terms % 2a—? ab-}- 
4, bb, or the Square of 3 4—5 b—} x x, which 
in the prefent cafe of finding the Logarithms 
-of Prime Numbers;.is always Unity, and cal- 
ding tbe Sum of the terms 4 zz -|-4 b==yy, the 
-Logarithm.of the ratio of / 2b to z4--3b or} 
_~ will be found 


Mt eg ty iB i I : 
eee Cale oie rest era &e. > 
“which ‘converges very much fafter than anly 
\ Theorem hitherto publithed for this purpofe- 
“Here note. ~ is all along applied to adapt thefe 


) aid | 


eye eT 


re et ORIN. LOO tod 9: ' it Rules 


44. Mifcellanea Curiofa, 
Rules to all forts. of Logarithms. If m be 
rocco &c. it may be neglected, and you will 


have JVapeir’s Logarithms, as was hinted be- _ 


fore; but ifyou defire Briggs’s Logarithms, 


which are now . general] 
divide your Series by |. 


Ret “TRO 
rae at how 3 


y received, you muft - 


2,302585092994045684017991 454684364207 


_ 60110148862377297603 3328 Dae 
or multiply it by the reciprocal thereof, #7z. 


©543429448190324518276511280189166050822 


94397003 803666 566114454-- 6) 


But to fave fo operofe a Multiplication 
(which is more than all the reft of the Work) 
‘itis expedient to divide this Multiplicator by 
the Powers of z or y continually, according to 
the Direction of the Theorem, efpecially where 
x 1s {mall and Integer, ‘referving the proper 
Quotes to be added together, when you have 
produced your Logarithm to-as many Figures 
as you defire: Of which Method fF will give 
a Specimen. fit 20 tes Lot gaey aay i 

If the Curiofity of any Gentleman that has 
leiftre, would prompt him to undertake todo 
the Logarithms of all Prime Numbers under 
¥00000, to 25 or 30 Figures, I dare affure him, 
that the facility of this Method willinvite him 
thereto 5 nor can any. thing more eafie be de- 
fired. And to encourage him, £ here give the 
_ Logarithms of the firft Prime Numbers under 

36 to 60 places, computed:by-the accurate Pen 
of Mr. Abraham Sharp, (from- whofe Induftry 
and Capacity the World may .in time expect 
great Performances) as they were ‘communi- 
“cated to me by our common Friend Mr. Euclid 


Speidall. ! 
Numb. 


— Mifeellanea Curiofa. 4s 


Numb. Logar ithm. 
2 0,30102999566398119521 373889472449 
3026768189881 462108541310427 
B Os47'7121254.719662.43729502790325511 
§ 3092001 283641 90695864329866 
J 0584509804001 425683071 221625859263 
«61 93.4835 7239632396 5406 503835 
TL 150413926851 §822504075019997124302 
} 42.4.1'706 70219046645 3094596539. 
13 1,11 3943352306837769206 54189502624 
* "6 254561189005053673288598083 | 
17 1 52304.48921 3782730285 4016989432833 
aif "1030007567378425046397380368 
AQ 1,27875360095282896153633347575692 
9317951 129337394497598900819 


‘The next Prime Rivgihee: IS '23; which. I will 
cake for an Example of the foregoing Dottrin, 


and. by the firft Rules, the Logarithm of the 


ratio of 22 to 23, will be pane to be either 


iG 2 SS espagnol bee teor 
aes 


I I 
os Be i I 119364 32181715 
Bec. 

“As likewife that of the ratio of 23 to 24 by 
a like Procefs. 


{ T ! ee + Bec 
E a 


ait aan! area t ssi 
&e. - And 


46  Mifcellanea Curiofa. 


And this is the Refult of the Dodrine of | 


Mercator, as improved by the Learned Dr. 
cee But by the fecond Theorem, wz. — 


ee sage &c. The fame Logarithms 


327 
a obtained gy ‘eye fteps. To wit, © 
Zag SEO Ca 
45 ' 273375 | 922640625 ' 2615686171875 
&c. and : | BoA ars 
2. a5 


ee a Te DT) TLL eee bee ee ness &C. 
47 31 1469 ° 1146725035." 3546361343241 


which was invented and demonftrated in the 
Hyperbolick Spaces Analogous to the Loga- — 


rithms, by the Excellent Mr. fames Gregory, 
in his Exercitationes Geometrice, and fince fur- 
ther profecuted by the aforefaid Mr. Speidall, 
in a late Treatife, in Englifh, by him publifhed 
on this Subjeé&. But the Demonftration as 
I conceive, was never till now perfe&ed with- 
out the confideration of the Hyperbola, which 
_ ina matter purely Arithmetical as this is, can- 


not be fo properly applied. . But what follows ~ 


Ithink 1 may more juftly claim as my Own, viz. 
‘That the Logarithm of the rae/o of the Geo- 
metrical Mean to the Arithmetical between 
22 and.24, or of / 528 to 23 will be foand t to 
be either. 


ee | PB ll a oe arava ft jie hos ee 


1058 ma ibeea + 395513 Sake 516487882248 
&e. or 


10§7 | 3542796379 1 $9676 58485285 
- All 


— Maifcellanea Curiofa. 47 
All theife Series being to be multiplied into 
044342944819 &c. if you defign to make the 

- Logarithm of Briges. But with great Advan- 
tage in refpect of the Work; the faid 434294 
4819, &c. is divided by 1057 and: the Quo- 
tient thereof again divided by three times the 
Square of 1057, and that Quotient again by 4 
of that Square, and that Quotient by ? there- 
‘of, and fo forth, till you have as many Figures 
‘of your Logarithm as you defire. As for Ex- 
ample; the Logarithm of the Geometrical 
Mean, between 22 and 24, is found by the Lo- 
garithms of 2, 3 and 11 to be | | 

| 10§7)43429 &c. 

3 in 1117249)41087 &c. 

4 in '1117249)12258 &c. 

Zin 1117249)65§832 &c. 

3 in 1117249)42088 &c. 

1.361 3169612669061 294500917 2669805 
( 41087462810146814347315886368 

Sede 12258521 544181829460074 

i heat 6583 235184376175 

iy ee nk" 

( 


4208829765 
Eig 
Summa. 


| 1.361 7278360175928788677771 1225117 


“Which is the Logarithm of 23 to thirty two 
places, and obtained by five Divifions with ve- 
ry finall Drvifors, all which is much lefs Work 
than fimply multiplying the Series into the faid 
' -Multiplicator 43429, &c. i | 
' Before I pafS on to the converfe of this Pro- 
“blem, or to fhew how to find the Number ap- 
pertaining 


43 Mifcellanea Curwofa. 
pertaining to a Logarithm afligned, it will be 
requifite to advertife the Reader, that there 
is a fmall miftake in the aforefaid Mr. ames 
Gregory's Vera Quadratura Circuli,& Hyperbole, 
publifhed at Padua Anno 1667. wherein he ap- 
plies his ‘Quadrature of the Hyperbola to the 
making the Logarithms; In pag. 48. he gives 
the Computation of the.Lord Napew’s Loga- 
rithm of 10, to five and twenty places, and © 
finds it. 230258509299404.5624017870 inftead 
Of 2302585092994045684017991,. erring inthe 
eighteenth Figure, as I was. aflured upon my 
own Examination of the Number L. here. give 
you, and by comparifon thereof with the fame 
wrought by another hand, agreeing therewith 
to 57 of the 6o-places. Being defirous to be 
fitisfied how. this difference arofe, I took the 
- no fimall trouble of Examining Mr. Gregory’s 
Work, and at length found, that in the infcri- 
bed: Polygon of 512. Sides, 5 in the eighteenth 
“Figure, was.a o inftead of 9, which being re- 
€tified, and the fubfequent _Work corrected 
therefrom, the refult did agree to a Unite 
-with our Number. - And this I propofe not to 
‘Cavil at an eafie miftake in managing of fo va 
“Numbers, efpecially by a Hand that has fo 
well deferved of the Mathematical Sciences, 
~“but.to-fhew'the exad& comcidence of two fo 
very differing Methods to make Logarithms, 
yaar ‘Might otherwife have’ been. queftion- 
~:°Ftom the Logarithm given to find. what 
ratio it expreffes, is a Broblem..that has not 
been fo much confidered.as the former, but 
- whichis. folved:with-the like eafe, and demon- 


a Mifcellanea.Curiofa. Ag 
ftrated by a like Procefs, from the fame gene- 
neral Theorem of Mr. Zvewton: For as the Lo- |. 
garithm of theratio of 1to1--7 was proved to be 
zs : ) 
19 
be Ae Y fo the Logarithm, which we 
will from henceforth call L, being given, 1--L, 
will be equal to itg\™ in the one cafe; and 
1-—L will be equal to al inthe other: Con- 


(my, and that of the ratio of 1 to 1—7 to 
24 


fequently 75-1)” will be equal to 1-19, and 
ae to 1—9; that is, according to Mr. 


“Newton’s faid Rule,. 1-|-mL-4~3 7m’ L?-|-4m3 L?-- 
tims -\-4.m°L? &c: will be==1-4-9, and 1— 
mL 4-3m*L? 2m L34- 4m? LAA, 3, mL? &e. 
will be equal to 1-9, m being any infinite In- 
‘dex whatfoever, which is a full and general 
Propofition from the Logarithm given to find 
the Number, be the Species of Logarithm what 
it will. But if MNapeir’s Logarithm be given, 
‘the Multiplication by m is faved (which Mul- 
fiplication is indeed no other than the redu- 
Pe ocre other Species to his) and the Series will 
be more fimple, vz. 1-|-L-}$LL43 L4--5L*4- 
Mey &cl of rol Lb shag $b sh 
4 €. This Series, efpecially in great Numbers 
converges fo flowly, that it were to be withed - 
it could be contracted. 


3 


a 


mr 


ms} OY 7 : 


50 Mifcellanea Curiofa. 


‘If one term of the ratio, whereof L is the 


Logarithm, be given, the other term will be. 


 eafily had by the fame Rule: For if L were . 


_ greater than the given L, and the difference ~ 


= 


Naperr’s Logarithm of the ratio of athe lefler 


to b the greater term, 0 would be the Produ& - 
of a into 1-pL-+$LL4"LLL &e. =4paL4 


aLL\eaL? &c. But if” were given, 2 would 


“be=?—bL-;-46LL—16L? &c. Whence, by the 


help of the Chiliads, the Number appertaining 


to any Logarithm will be exactly had to the © 
utmoft extent of the Tables. If you feek the 
neareft next Logarithm,whether greater or lef- | 


fer, and call its Number a if lefler, or 0 if 


thereof from the faid neareft Logarithm you 


call /; it will follow, that the Number an- 
fwering to the Logarithm L will be either a © 


into. 1-}-/- 51 gl El’ &e. or elfe b 
into 1—/-{|-4ll—s1L-b + ,75/* &c. wherein as 
his lefs, the Serzes will converge the fwifter. | 
And if the firft 20000 Logarithms be given to © 
fourteen Places, there is rarely occafion for 


the three firft fteps of this Serzes to find the 
Number to as many places. But for Ulacq’s. 
great Canon of 100000 Logarithms, which is: 
made but to ten places, there is fcarce ever. 
need for morethan the firft ftep 4-| a/ or a-- 
malin one cafe, or'elfe b—b1 or b—m b/ in 
the other, to have the Number true to as ma-_ 


ny Figures as thofe Logarithms confift of. 


If future Induftry fhall ever produce Loga- 
rithmick Tables to. many more places than. 
now we have them; the aforefaid Theorems. 


will be of more ufe to reduce the correfpondent 
Natural Numbers to all the places thereof. 
In-order to make the frit Chiliad, ferve all 

‘Utes, 


— Maifcellanea Curiofa. 51. 
Jfes, I was defirous to contra this Series, 

wherein all the powers of J are prefent, into 

fone, wherein each alternate Power might be 

wanting ; but found it neither fo fimple or 

uniform as the other. Yet the firft ftep there- 
f is, I conceive, moft commodious for Prac- 

tice, and withal exa@ enough for. Numbers 

not exceeding fourteen places, fuch as are 

Mir. Brigs’s large Table of Logarithms; and 

herefore I recommend it to common Ufe. 

b> It is thus 2 a-- Go! or b— sel 

i} | oe eer: 


vill be the Number anfwering to the Loga- 
ithm given, differing from the Truth by but 
me half of the third ftep of the former Series. 
ut that which renders it yet more eligible, 
that with equal facility, it ferves for 

wg’s Or any other fort of Logarithm, with 


7 ‘a uae oe ee T ° - 
he Only variation of writing — inftead of 1, 


: at is, a-|- 


a : b! 1 i. 
— and b— oe gets 
aa ae ——— and 
2 


i. | 
? which are eafily refolv’d into A- 


As 43429 &¢e.—2/ to 43420+-5/ : -1 to the 


So is 2 { Num- 
43429 &e.|-3! to 43429— $12: ae 


E 2 If 


CE ar i Lys 
‘ vale ies bs decid BB i Bey ye 


52 Mifcellanea Curiofa. 
If more fteps of this Series be defired, it 


Ls Me ‘ al 4.al> 
will be found as follows, a ieee a 


1 als ; ‘ , id | ; 
Saey &c. as may eafily be demonftrated by 


working out the Divifions in each ftep, 
and collecting the Quotes, whofe Sum will be 
found to agreee with our former Series. 
Thus I hope, I have cleared up the Doc- 
trine of Logarithms, and fhewn their Con- 
ftruction and Ufe independant from the Ay- 
perbola, whofe Affections have hitherto been 
made ufe of for this purpofe, though this be a 
matter purely Arithmetical, nor properly 
demonftrable from the Principles of Geome- 
try. Nor have I been obliged to have re- 
courfe to the Method of Indivifibles, or the 
Arithmetick of Infinites, the whole being no 
other than an eafie Corollary to Mr. Newton’s 
General Theorem for forming Roots and 
Powers. : | rs 


| Mifcelanea Curtofa. 53 


A SOLUTION, 


Given ty Mr. ‘fohn Collins, of a Choro- 
_ graphical Problem, Propofed by 
Richard yoraicy, Eiq; 


PROBLEM. 


TheDiftances ofthree Objectsin the © 
fame Plain being given, as 4,B, 
C; The Angles made at a fourth 

e Place in the fame Plain as at 

8, are obferved : The Diftances 
from the Place of Obfervation 
to the refpective eae are re- 
quired. 


The Problem hath fix Cafes. 


Caf 1. ¥ F the Station be taken without the 
Triangle made by the Objects but 
inone of the fides thereof produced, as at Sin 
the orh Figure; find the Angle ACB; then 
in the Triangle "ACS all the Angles and the 
fide AC are known, whence either or both the 
Diftances SA or SC ie be found. 


ae Bs Gea 


5 4. Maifcellanea Corfe | | 


Cafe 2. If the Station be in one of the Sides 
of the Tt iangle, as in the roth Figure at Sy. } 
then having the three fides AC, CB, BA given, 
find the Angle C_4 B; then again in the Tri-” 
angle SA B, all the Angles, and the fide AB, 
are known; ence may be found either 4S, 
or SB, Geometrically, if you make the “Angie. 

CAD equal to the obferved Angle c S B, and 
draw BS parallel to DA, you determine the 
Point of Station S. 

Cafe 3.1f the three Obj edtslie in a right Ling! 
as ACB (fuppofe it fone and that a Circle 
pafleth through the Station S, and thetwo ex- 
terior Objects A B, then is the Angle ABD 
equal to the obferved Augle A sc. (by 21 of 

_ the 3d Book of Euclid) as infifting on the fame 
Arch AD: And the Angle BAD in like 
manner equal to the obferved Angle c SB: 
By this means, the point D is determined. 
Join DC, and produce the fame, thn a Circle 
pafling through Points A B D, interfedts Dc, 

: produced at S, the place of Station. 


Calculation. 


In the Triangle 4 B D, all the ovine: and 
the fide 4 Bare known, whence may be i 
the fide 4 D. 

Then in the Triangle C_A D the two fides 
c A and AD are known and their contained 
Atigle c AD is known ; whence may be found 
the Angles cD A and ACD, the comple- 
_ ment whereof to a Semicircle is the Angle $ 
cA: in which Triangle the Angles are now 
all known and the fide 4C: whence may be 
found either of the Diftances, SC or Sale 

| Cafe + 


WF ee ees Sy 
mah x van 


: Mifcellanea Curiofa. | 55 


angle, made by the Objects, the fum of the 
Angles obferved is lefs than four right Angles. 
The Conftruction is the fame as in the laft 
Cafe, and the Calculation likewife ; faving 
that you muft make one Operation more, ha- 
ving the three Sides, 4C, C B, BA, thereby 
find the Angle cA B, which add to the Angle 
E AD, then you have the two fides, viz. A 
C, being one of the Diftances,and 4 D, (found 
as in the former Cafe) with their contained 
Angle C_AD, given to find the Angles CDA, 
and 4 C D, the Complement whereof to 4a Se- 
micircle, is the Angle SC 4: Now inthe Tri- 
angle Sc.4, the Angle at c being found, and 
at S obferved, and given by Suppofition, the 
other at 4 is likewife known, as being the 
complementof the two former to a Semicircle, 
and the fide 4 C given ; hence the Diftancec S 
or 4S may be found. 


- Cafe 5. If the place of Station be at. fome 
Point within the plain of the Triangle, made 
by the three Objects, the Conftruction and 
Calculation is the fame as in the laft, faving 
only that inftead of the obferved Angle 4 Sc, 
the Angle 4 B Dis equal to the Complement 
thereof to a Semicircle, to wit, it is equal to 
the Angle 4 SD; both of them infifting.on the 
fame Arch 4D: And in like manner the An- 
sie B 4D is equal tothe Angle DS B, which 
is the Complement of the obferved C S B; and 
in this Cafe, the. fum of the three Angles ob- 
ferved,: 1s equal to four right Angles. 


B 3 In 


Cafe 4. If the Station be without the Tri- 


‘ 


Biss aie tS gat 


56 Mi fc dee Curio ip a. 


In thefe three latter Cafes no ufe is oN of | 


the Angle obferved.between the two Objects, © 


as 4 and B, that are made the Bafe-line of the 
Conftr uétion : ; yet the fame is of ready ufe for / 
finding the third Diftance, or laft fide fought, 
as in the fourth Scheme, in ‘the Triangle S 4 2B, 
theré is given the Diftance 4 B, its oppofite- 
Angte equal to the fum of the two obferved 
‘Angles, and the An@le S 4B attained, as in 
the fourth Cafe: Hence the third Side or laf 
Diftance SB may be found. 

And here it may be noted, that the three 
Angles C 4S, 4S 8B, SBC, are together equal 
to the Angle ACB, "for the two Angles c SB, 
and Cc BS, are equal to ECB, as being the 
Complement of SC B to two right Angles; and 
the like in the Triangle on the other em 
EPS OPO ET 


Cale G2 IE the diget Objeas be' 4, B,C, anid 


the Station at S, as before, it may happen, ac= 


‘cording to the former Conftructions, that the 
Points C and D may fall clofe together, and 
fo a right Line joining them may be produced 
with uncertainty : ; in fach cafe the Circle may 
be conceived to pafs through the place of Sta- 
tion at S, and any two of the Objects (as im 
the fixth’ Scheme) through Band C; wherein 
making the Angle DBC équal to the obferved 
Angle A Sic} and Bt D equal to the Comple- 

tment to 1 80 degrees of both the obferved An- 
gles in DSB thereby the Point D is determi- 
ned, through which, and the points cB, the 

Circle isto be defcribed , and joyning D 4, 
(produced, when 5 requireth) where it in- 

BP: asic: 


a 


i 
1 


% 


ce em 
SR a ea a j 


K Plater, pape 87 


Cine: 


i Mifeellanea Curiofa. Hee 37 


Be eitetts, the Circle, as at S, is the place of Sta- 
coe fought. 


ig This Problem may be of oond Ufe for the 
_ due Situation of Sands or Rocks, that are 
within fight of three Places upon Land, whofe 
 diftances are well known; or for chorographi- 
cal Ules, &c. Efpecially now there isa Me- 
- thod of obfervingAngles nicely accurate by aid 
of the Telefcope ; and was therefore thought fit 
to be now Publifh’d though it be a competent 
time fince it was delivered in Writing. 


The 


‘ad ha "s TE ETE RT a ae ee 
¥ : s + = ae ay ee 
j A i 


a Maifcelanea Curiofa. ae oe 


| The Solutions of three Chor oer aphic 

- Problems, by a Member of the 
Philofophical Society of Ox- 
ford. ce 


HE three following Problems may 
occur at Sea, in findimg the diltance 
and pofition of Rocks, Sands, &c. from the Sea 
Shoar; or in the Surveying of the Sea Coaft ; 
When only two Objects, whofe diftance from 
each other is known, can be feen at one Sta- 
tion ; but efpecially they may be ufeful to one 
that would make a JZap of a Country bya 
Series of Triangles derived from one or more 
~meafured Bafes ; which is the moft.exact way 
of finding the bearing and diftance of Places — 
from each other, and thence their true Lon- 
gitude and Latitude; and may confequently 
occur to one that would in that manner mea- 
fure a Degree on the Earth. vs 


The firft Problem (Fig. 3 and 4.) 


There are two Objects, B and C, whofe di- 
ftance BC is known; and there are two fta- 
tions at .4 and E, where the Objetts Bc 
being vifible, and the Stations one from 
another, the Angles BaC, B4AE, AES, 
A Ec, are known by Obfervation, (which 
may be made with an ordinary Serveying Se- 
micircle, or Croftaf, or if the Objects be 

beyond 


Mifcellanea Curiofa. 9. 
beyond the view of the naked Eye, with a 


- Telefeopick, Quadrant) to find the diftances or 
lines AB, AC, AE, EC. | 


ee Conftrution. 

In each of the Triangles BAE, CAE, 
two Angles at -4, E, being known, the third 
is alfo known: then take any line #¢ at plea- 
fure, on which conftitute the Triangles Bas, 
a¢y refpectively equiangular to the Triangles 
BAE, AEC; join8y. Then upon BC con- 
ftitute the Triangles BC A, BCE, equiangu- 
lar to the correfpondent triangles By, By, 
_ join AE, and the thing is manifeftly doge. © 


Tie Calculation. 

Affuming #¢ of any number of parts, in 
triangles « B¢, ey, the angles being given, 
the fides «8, “¥,¢8,2y may be found by 
Trignometry: Then in the Triangle pay, 
having the angle 824, and the legs af, 7, 
“wemay find @y. Then By. BC:: 2a, BA: 
Pees ya Cas yt Cr. 


The fecond Problem (Fig. § and 6.) 


_ Three Objedts B, C, D, are given, or (which 
is the fame) the fides, and confequently an- 
sles of the triangle BCD are given; alfo 
there are two points or ftations A, E, fuch, 
that at 4 may be feen the three points BCE, 
but not D; and at the ftation E may be 
feen .4,C,D, but not B, that is the angles 


me PAC, BAE, AEC, AED, (and confe- 


quently E AC, AEC, are known by obferva- 
Ween; co find the lines 48, 0, AE EC, 
L ED. Con- 


60 = Mifcellanea Curiofa. 


— Conftruttion. gic 
Take any line ¢ at pleafure, and at its ex- 
tremities make the angles «ey, #8, aeyz, 


aed equal to the correfpondent obferved an- 


Bless EAC, EAB, AEC, AED. Produce & 2, 


#<, till they meet in?, joing»; then upon 
CB deferibe (according to 33. 3. Eucl.) a feg- 
ment of a circle that may contain an angle= 
¥¢B6; and upon CD defcribea feoment of a 
Circle capable of an angle=7 9S; fuppofe F 
the common fection of thefe two circles ; join 
FB, FC, FD; then from the point C, draw 
forth the lines C_4, CE, fo that the angle FCA 
may be==? 7 2, and FCE==97¢; fo A, E, the 
common Sections of CA, CE; with FB, FD, 
will be the points required, from whence the 
reft is eafily deduced. 


The Calculation. 
Affuming «¢ of any number, in the trian- 


gles yt, #%¢, all the angles being given, ~ | 


with the fide #¢ aflum’d, the fides « >, ¢ ¥, ?, 
29, will be known; then in the triangle 7 29, 
the angle 7 #?, with the legse7, +9, being 
known, the angles «97, 279, with the fide 
®y will be known: then as for the reft of the 
work in the other figure, the triangle BC D 


having all its fides and angles.known, and the ~ 


angles BFC, BF D, being equal to the found 
Bey, 894; how to find FB, FC, FD by Cal- 
Culation (and alfo Protrattion) is fhewn by Mr. 
Collizs in the precedent Difcourfe, as to all 
its cafes, which may therefore fuperfede my 
fhewing any other way. ae ne 


But 


Mifcellanea Curiofa: 64 
But here it muft be noted, that if the fim 
of che obferved angles, B AE, AED, is i180 
degrees : then 42 and E D cannot meet, be- 
caufe they are parallel, and confequently the 
given Solution cannot, take place ; for which 
reafon I here fubjoin another. 


Another Solution me | 
Upon Bc (Fig. 7.) defcribe afegment BAC 
of a circle, fo that the angle of the fegment 


may be equal to the obferved 4827, (which 


as above quoted is fhewn 33. 3. Euclid.) and 
upon CD defcribe a fegment C E D of a circle 
capable of anangle equal to the obferved CED; 
from c draw the diameters of thefe circles cG 


cH; then upon cG defcribe a fegment of a 


circle G FC, capable of an angle equal to the 
obferved L AEC; likewife upon c Hdefcribe 
a circle’s fegment c FH, capable of anangle 


% equal to the obferved c 4E: fuppofe F the 


common Seétion of the two laft circles HF c, 


GFC, join FH, cutting the circle HEC in E, 


join alfo FG, cutting the circleG AC ina: } 

fay that 4, Z, are the points required. 
Demonftration. 

“For the LB 4C is=gay by conftruction of 

the fegment, alfo the angles cE H, C 4G, 

are right, becaufe each exifts in a femicircle: 


- therefore a circle being defcribed upon C F as 
a.diameter, will pafs through E, 4; There- 


fore the angle C4 E==-L cFE=C pi=(by 
conftruction) to the obferved angley¢*. In 
like manner the LC E A==c F 4c FG= ob- 


 ferv’d qarte y 6 te 


In the ftations 4, F, fallin a right line with 
the point C; the lines G 4, HE being paral- 
i Sie | | le}, 


62 Mifcellanea Curiofa. 

lel, cannot meet: but in this cafe the Problem 
is indeterminate and capable of infinite Solu-. 
tions. For as before upon CG defcribe a Seg- 
ment ofa circle capable of the obferved Ly: «, 


and upon C H, defcribe a Segment capable of — 


the obferved 72¢: then through c, draw a 
line any way cutting the circles in 4, E, thefe 
points willanfwer the queftion. | 


The third Problem. 


Four points B, C,D,F, (Fig. 8.) or the 4 fides 
of a quadrilateral, with the angles compre- 
hended are given; alfo there are two ftati- 
ons:4 and E fuch, that at-4, only 8.0 2 are ~ 
vifible, and at E only ADF, that is, the 
angles BAC, BAE, AED, DEF are given: 
to find the places of the two poiuts 4£, and 
confequently, the lengths ofthe lines 4B, AC, 
AE, ED, EF. : 

Conftruttion. a) 

Upon BC (by 33. 3. Eucl.) defcribe a feg- 
ment of a circle, that may contain an angle 
equal to the obferved angle BAC, then from 
C draw the Chord C 4%, or a line cutting the — 
circle in 77; fo that the Angle BCA4 may 
be equal to the fupplement of the obferved 
angle BAE, 1. €. its refidue to 180 degrees. 
In like manner on D F defcribe a fegment of 
a circle, capable of an angle equal tothe ob- 
ferv’'d DE F,and from D draw the Chord DN, 
fo that the angle F D N may be equal to the 
fupplement of the obferv’d angle 4 £F, join 
MN, cutting the two circles in 4,£: I fay — 
/, ®, are the two points requir’d. 


Demone 


—Mifeelanea Curwfa, 62 

7 | Demonftration. aed 
Join 48,40, ED, £F, thenisthe £ ACAB 
LBC (by 21.3. Eucl.)= fupplement of 
the obfervd 4 8 4 E by conftrution, therefore 
the conftructed 4 8 4 £, is equal to that which © 
was obferved. Alfo the 4 BaCof the feg- 
- ment is the’conftruction of the Segment, e-. 
' qualtotheobferv’'d £3.4c. In like manner 
the conftruéted angles 4EF, and DEF,-are 
equal to the correfpondent obferved angles 
AEF, DEF, therefore 4£ are the points re- 
guir’d. Pith 
‘ The Calculation: | 
_- In the Triangle BC AZ, the L Bc 24 (=fup- 
_ plement of B4£) and 4B AIC (= BAC) are 
_ given, with the fide Bc ; thence A¢C may be 
found; in like manner DNinthe ADNF 
may be found. But the 4 AfcD)=3 cD--- 
- pC M)is known,with its legs 74.c, c D> there- 
fore its Bafe A7D, and LA7DC, may be 
known. Thereforethe LDN (=cDF.- 
CD M--F DN) is known, with its legs Mp, 
DWN; thence MN with the angles DMN, 
DNM, willbe known Then the4cMA(= 
(LDMC --D MN) is known, with the MAC 
==MAB+B4AC): and MC before found ; there- 
fore MA and 4c will be known. In like 
manner in the triangle E DN, theangles £, Nn, 
- with the fide D N-being known, the fides EN, 
ED, will] be known; therefore 4 E (= M N--- 
_ M4A--EN) is known. Alfo in the triangle 4 
ec, the 4 A with its fides BC, C 4, being 
- known, the fide 4 2B, will be known, with the - 
 £8c 4310 inthe triangle £ FD, the 4 £ with 
- the fides, ED, DF being known, EF will be 
found, with the LEDF. Laftly, in the Fas 
gle 


OE a aT eRe 4 

64 Maifcellanea Curiofa: 
gle Ac D, the L AC D (SBC D--BC 4) with 
its legs 4C, c D being known, the fide 4 D, 
will be known; and in like manner EC in the 
triangle EDC. ae 

Note, that in this Problem, as alfo in the 
firft and fecond, ifthe two ftations fallin a 
right line with either of the given Objeds: 
the locus of 4, or E, being a circle, the par- 
ticular point of 4, or E, cannot be determined © 
from the things given. ae 

Asto the other cafes of this third Problem, 
wherein 4 and £, may fhift places, 7.e. only 
_DFE, may be vifible at 4, and only 4, B,c, 
at E; or wherein 8, .D,E, may be vifible at 
A, and only c, F, 4, at E; or wherein 4 may 
be of one fide of the quadrilateral, and E on 
the other; or one of the ftations within the 
quadrilateral, and the other without it: I 
fhall for brevity fake omit the Figures, and 
diverfity of the Sines ~- and-- in the caleula- 
tion, and prefume that the Surveyor will ea- - 
fily direé&t himfelf in thofe cafes, by what has 
been faid. ly th 

The folution of this third Problem is gene- 
ral, and ferves alfo for both the precedent. 
For fuppofe ¢ D, the fame point in the laft f- 
gure, and it gives the folution of the fecond — 
Problem: but if BC be fuppos’d the fame 
points with D, F, by proceeding as in the laft, 
you may directly folve the firft Problem. 


a 7 ae Tea 
+ Fe eae eng 


Mifeelanea Curtofa. 65 


Aa Arithmetical Par ‘ad ox, concern-. 
tg the Chances of Lotteries ; by 
aie Honouradle Francis Roberts, 


ere Fellow of the R. 5. 


S fome Truths (like the Axioms of Geo- 

metry and Afetaphyficks) are felf-evident 
at the firft View, fo there are others no lefs 
certain in their Foundation, that have a very 
different Afpect, and without a ftri@ and care- 
‘ap Examination, rather feem repugnant. 

We may find Inftances of this kind in moft 
‘Sciences. t 
_ In Geometry, That a Body of an infinite 
poet, may yet have but a finite Magni- 
tude ¢ 
In Geography, That if Axtwerp be due Eaft 
to London, for that reafon London cannot be 
Weft to Amvwerp. 

In Affronomy, That at the Bardadoes (and 
‘other Places between the Line and Tropick) 
‘the Sun, part of the Year, comes twice ina 
Morning to fome Points of the Compafs. 

Jn Hydroftaricks, That a hollow. Cone (ftand- 
‘ing upon its Bafis) being fill’d with Water, 
the Water hhall prefs the bottom with three 
times the Weight, as if the fame Water was . 
frozenito Ice ; and Figures might be contriv’d 
to make it aha a hundred times as much. 


, SaaS j ’ 
. nat Bt; The 
¥4 


See ars ae 


| ” 

66 Mifcellanea Curtofa. 
’ Thefe Speculations, as they are generally — 
pleafant, fo they may alfo be of good ufe to 
warn us of the Miftakes we are liable to, by 
carelefs and fuperficial Reafoning. ns 
I fhall add one Inftance in Arithmetick,which 
perhaps may feem as great a Paradox as any 

of the former. ? 

There are two Lotteries, at either of which 
a Gamefter paying a Shilling for a Lot or 
Throw; The firft Lottery upon a juft Com- 
putation of the Odds, has 3 to 1 of the Game- 
{ter ; the Second Lottery, but 2 to one ; ne- 
verthelefs, the Gamefter has the very fame 
difadvantage (and no more) in playing at the 
Firft Lottery, asthe Second. 3 

It looks very like a Contradiétion, that the: 
Difadvantage fhould be no greater in playing 
againft 3 to 1, than 2 to1, but it may thus be: 
refolv’d. . | i 

io) 


a € f-) ps S70 . 16 pence 
ie 8s 4 a-piece. 

a) ° ie ; 
wo \- 8 ip. a yas a, ©2 fhilling ogee 


In the firft Lottery the Gamefter hazards a’ 
Shilling to win a Groat, and the Chances be- 
ing equal, it is evident there is 3 to one againft 
him. : ek: 

In the Second Lottery, the Gamefter ven- 
tures a Shilling againit a Shilling,and the Lots 
being 4 to 2, his Difadvantage is 2 tor. | 

And a Lot at either of them being truly 
worth juft 8 Pence, (viz. the 6th part of 3 
times 16 Pence, or twice 2 Shillings) the Dif-' 
advantage muft be the very fame in both Ca-’ 
fes, that is, the Gamefter pays a Shilling for. 
a Lot that is worth but 8 Pence. e 

: @. 


Maifcelanea Curiofa. 67 
The Method of finding this Anfwer being 
mewhat out of the common Road, I fhall 
re add it, and thereby infinite Solutions of 
e fame kind may be difcovered. | 


if. Lottery. 


_ Let a=the number of Blanks 
b—the number of Prizes. 
v==the Value of a Prize. 


2d. Lottery. 


_ Let m=the number of Blanks. 
n==the number of Prizes. 
s=the value of a Prize. 


=to what you pay for a Lot,vz. a Shilling. 


$0 the Lottery has its Chances for 1, and 
'Gametfter his for y—1. Now the true Odds 
uifting of the compounded Proportion of 
"Chances and the Values, ox. F-and >. 
‘Share of the Lottery will be z, and that of 
:Gamefter r4—b. Therefore as the pre- 
t cafe ftands, the firft Lottery muft bea=3 — 
-3b, and by the like reafoning, the fecond ': 
ttery will be m=2 sx—2n”. Now the Value © 
| Lot being the Sum of the Prizes divided — 
the-number-of-Lots, (which muft be equal 
0th Lotteries) it yields i a 
a ae 

1M SH ‘ 
$ car ape m-\-70 % 


ee: 30 


68 Mifcellanea Curtofa. a | 


| 14 = 3rb—3b 
b 2m= 2sn—2n 

| rb s2 
¥ ae? | 3a +b mye 
m | . | AC) 
” 5\(*) 
s J Cx) : : 

RET NE | 
= t 0. | 
7* ab ee yb q 
: 


Scope j bai ‘ 
11, of alte aczo to avoid negative Numbers. 


135 3 13°36 = 3qb. he Re hee 
12,14 |i4qel | 7 
coe _ {15'g D>1 makesa < 0,g— 1 makes 2 > 


seasonal 
Scope | 
is 4 16 |16lfb=o 
17 + 34117394 m4 
16,18 N8qok 


[191g <2 makes <o q > y makes b 
—_————— 


be fe A 
397 Pntn 4 

20% m-\-m1o 1 \sn = qm-|-qu 

21% 2 |o9\2sn =2qm-|-2qn 

24-27 ‘loslesmmm-2ng—w 

22, 23. |o4\2qm-|-2qu = m-[-2n 


Scope aslif m =o 
24, 25 426/2q”2 = 2n 
26-r2n 127951 es 
as, 27 1284 >> 1makesm <0 q< 1 makesm 


Ne > ~ 
~~ = 


- Mifeellanca Curiofa. | e 


A (29, 1f 2 = 0 

24,29 BO2qmmm 

“30 >2m Iiqmui 

29, 31 ME pahegy — o Peat 0 


33,4 4 (*)|34| Let vai nue Qa: 


7 ee 
ab 3 
me a 10136) a yh = 24-|-26 = a-}- 36 
: —- Blianb 
20; 34. 38 Ss at 2 
‘ Q * Aw, 143 
3 +5 77 350 & 2m-\- 20 
.3? 49. 6sn = 4m-\-4n 
+ 23 *F lWti6m= 3m-6n 
4°, AF 


bes qm-*-4n = 3m-|6n 


42— 13) ma an 
; 1537 [441 = 3r—3 
Baas | [+5 37 = 4 
45 +2" 47 sabes 
5 (*) [18]Let 4= 
37, 48 [19/8 = 
| 45 +3 {,0X4=4, id eft, 16 Pence. 
be 6 (*) st! Let Mm 4 
43> 51 52! N= 2 ; 
mage 2 153 S$=2> 2 Shillings 
ob 
+ B 3 


: Se 
A New, Exatt-and Hafie Method, 
of finding the Roots of any Equa- 
tions Generally, and that wnt hout 
any previots Reduction. By Hdm. 


Halley. 


a5 HE principal ufe of the Avzalytick Art, 
is to bring Mathematical Problems to 
Equations, and to exhibit thofe Equations in 
the moft fimple Terms that can be. _ But this 
Art would juftly feem in fome degree defe- 
 étive, and not /ufficiently Analytical, if there 
were not fome Methods,by the help of which, 
the Roots (be they Lines or Numbers, might 
be gotten from the Equations that are found, 
and fo the Problems in that refpedt be folved. 
The Ancients fcarce knew any thing in thefe 
Matters, beyond Ouadratick Equations. And 
what they writ of the Geometrick, Construction 
of folid Problems, by the help of the Parabola, 
_ Ciffid, or any other Curve, were only patti- 
cular things defign’d for fome particular Ca- 
fes. Butas to Numerical Extradiop, there is 
every where a profound Silence; fo that what- 
ever we perform now in this kind, is entirely 
owing to the Inventions of the Moderns. 

And firft of all, that great Difcoverer and 
Reftorer of the Modern Algebra, Francu Viet ay, 
about 1co Years fince, fhew’d a general Me- 


i 


Mifcellanea Curiofa. 71 
thod for extraGing the Roots of any Equati-. 
on, which he publifh’d under the Title of, 4 
Numerical Refolution of Powers, &c. Harriot, 
Oughtred, and others,as well of our own Coun- 
try, as Foreigners, ought to acknowledge 
whatfoever they have written upon this Sub- 
jet, as taken from Vietz. But what the Sa- 
-gacity of Mr. Newton’s Genius has perform’d 
in this bufinefS,we may rather conjecture (than 
be fully affur’d of) from that fhort Specimen 
given by Dr. Wallis in the 94th Chapter of his 
Algebra. And we muft be forced to expedt it, 
till his great Modefty hall yield to the Intrea- 
ties of his Friends, and fuffer thofe curious 
Difcoveries to fee the Light. 

- Not long fince (viz. A. D. 1690) that ex- 
cellent Perfon M. Fofeph Raphfon, F. R.S. pu- 
blift’d his Uxiver{al Analyfis of Equations, and 
illuftrated his Method by plenty of Examples; 
by all which he has given Indications of a 
Mathematical Genius, from which the great- 
eft things may be expected. 
_. By his Example, M. de Lagney an ingenious 
Proteffor of Mathematicks at Paris, was en- 
courag’d to attempt the fame Argument, but - 
he being almoft altogether taken up in ex- 
tracting the Roots of pure Powers (efpeci- 
ally the Cubick) adds but little about affected 
Equations, and that pretty much perplex’d 
too, and not fuficiently demonftrated. Yet 
he gives two very compendious Rules for the 
Approximation: of a Cubical Root; one a 
Rational, and the other an Irrational one. 
Ex. gr. that the fide of the Cube aaa}-b, is 
between 
ry 


eh tee Rs ee Deak tb Vide 
° The an 
ee 


72 gto — ) 
Aa coal 344a- —— & Neue art --- 4 a4 


And the root of the sth Power a $4 b, sh: 
makes 


we Viet z a pea Note, that 


tis 4 aa, not 2 ie as ’tis erroneoufly Printed 
in the Py ench Book) Thefe Rules were com- 
municated to me. by a Friend, I having not 
feen the Book ; but having by tryal found the 
goodnefs of them, and admiring the Compen- 
dium, I was willing to find out the Demon- 
ftration- Which having done, I prefently 
found that the fame Method might be accom- 
modated to the Refolution of all forts of Equa- 
tions) And I was the rather inclin’d to im- 
_ prove thefe Rules, becaufe I faw that the 
whole thing might be Explain’d ina Synopfis s 
and that by this means, at every repeated: 
ftep of the Calculus, the Figures already found 
ya the Root, would be at leaft Trebled, which 

U other ways, are encreafed butin an equal 
Number with the given ones- Now, the fore- 
mention’d Rules are eafily demonftrated 
from the Genefis of the Cube, and the sth 
Power. For, fuppofing the fide of any Cube 
rate, the Cube arifing from thence, 1s asa-- 
344¢. £3 zee-|-eee. And confequently, if we fup- 
pofe zaa the next lefs Cube, to any given Non~ 
cubick Number, then eee will be lefs than 
Unity, and the remainder 6, will = the 
other Members of the Cube, saber 3.a€e-|-e¢e. 
Whence rejecting eee upon the account of its 


fmallnefs, we have os ace ina And fince 
| ae 


Maifcellanea Curtofa. 73 
aae is much greater than aee, the quantity - 
will not much exceede; fo that putting 


e = —- then the quantity —-——(towhich 
3aa 3 4a-\-3, ae : 


e is nearly equal) will be found 


b b . ab 
ey ih eee or ——-—— that is ——, =, 
34a\-3ab 3aa+-b 344a4+-b 
gaa? Dee 


And fo the fide of the Cube aza--s will be 
“T Saa-) : 

M. de Lagney. But now, if aaa were the next 
greater Cubick Number to that given, the fide 
of the Cube aaa—b, will after the fame man- 


ab 
Fe Pan And this eafy 


and expeditious Approximation to the Cubick — 
Root, is only (a very fmall matter) erroneous 
in point of defect, the quantity e, the remain- 
der of the Root thus found, coming fomething 
lefs than really ’tis. 
As for the/rratiovale Formula, tis deriv’d from 
the fame Principle, vz. b= 34ae--3aee, or 


which is the Rational Formula of 


ner be found to be 4«— 


b 
—_ = aelee, and fo V { aa aa é = 241-e, and 
pa ae oe ag ; 


/ / rs? |.ja=a+e, the Root fought. Alfo 
¥ 34 
the fide of the ‘Cube aaa—b, after the fume 


aero _| 


manner, will be found to be bat taa— b 


aif M ifcellanea Curiofa. 


And this Formula comes fomething nearer to 


the Scope, being erroneous in point of exce/s, 


as the other was in defeé, and is more accom- 
modated to the ends of Pra¢tice, fince the Re- 
ftitution of the Calculus, is nothing: elfe but 
the continual addition or fubftraGion of the 
A aee LL ) VI peer ay 
Quantity according aS the quantity e can 


be known. © So that we fhould rather write 


2 ‘ —~€£CL ee — ; bl / a 
/ bail |-ta; in the former.cafe, and in 
| 34 


the latter, say va pss, But by cither 
of the two Formulas, the Figures already 
‘known inthe Root to be extracted, are. at 
teaft Tripled; which I conclude will be very 
grateful to-all the Students in. Arithmetick ; 
and I congratulate the Inventor upon the ac- 
‘count of his Difcovery. Bt 
But that the ufe-of thefe Rules may be the 
better perceiv’d, I think it proper to fubjoin 
an Example or two. Let it be propos’d to 
find the fide of the double Cube, or aaa--b=2. 


b 
Here 4=1, and a = 7:&f0! -- /72,0r 1, 26, 


be found to be the true fide nearly. Now, the 
Cube of 1, 26, is 2,000376, and fo 0,63 +4- 


\/'23969—32000376 | oF 0, 63 ty/, s9680052 
ee as | 
9100§291 = 1,259921049895--3 which in 13 
Figures, gives the fide of the double Cube, 


with very little trouble, viz. By one only di- 


vifion,-and. the extraction of the fquare' Root; 
when as by the common way of working, how 
Dil much 


A, 
ak 


REE Lin) 


Mifcellanea Curiofa. 75) 


much pains it would have coft, the Skilful — 
very well know. This Calculus a Man may. 
continue as far as he pleafes, by encreafing the. 


Square by the addition of the quantity - ts 


which Corredion, in this cafe will give, but. 


the encreafe of Unity in the 14th Figure of 


the Root. 

. Exemp. 2d. Let it be propos’d to find the 
fides of a Cube equal to that Englifh Meafure 
commonly call’d a Gallon, which contains 231. 
folid Ounces. The next lefs Cube-is 216, 
whofe fide 6= 4, and the remainder 15 =4 ; 
and fo for the firft Approximation, we have 


s+-V 91-5 — the Root. And fince /9,8333... 


is 3,1358..., “tis plain that 6,358 4+-e. 
Now, let 6,1358=2;and we fhallthen have for 
its Cube 231,0008 5 3894.712,&according tothe 
Rule,3,0679'b-v/9, 41201041—, 000858394712, 
OES AOTO 
is moft accurately equal to the fide of the gi- 
ven Gube, which within the fpace of an Hour, 
I determin’d by Calculation to be 6.1357924 
3966195897, whichis exactin the 18th Figure, 
defeGtive in the roth. And this Formula is 
defervedly preferable to the Rationale, upon 
the account of the great Divifor, which is not 
to be manag’d without a great deal of Labour; 
whereas the extraction of the fquare Root, 
proceeds much more eafily, as manifold Ex- 


_. perience has taught me. 


But the Rule for the Root of a pure Surfo- 
lid, or the 5th Power, is of fomething a higher 
Enquirv, and does much more perfectly yet, 

do. 


itl Shea a oh ot ABS i ma 
re 3 


76 |) Mifcelanea Curiofa. — 

do the bufinefs; for it does at leaft Quintuple 
the given Figures in the Root, neither isthe — 
Calculus very large or operofe. Tho’ the Au- 

thor no where fhews his method of Invention 
or any Demonftration, altho’ it feems to he 
very much wanting ; efpecially fince all things 
are not right in the printed Book, which may 
eafily deceive the Unskilful. Now the sth 
power of the fide 2+e is compos’ of thete 
Members, 4°-\52*e|-10@3e” -|-10a*e3-|- 5. ae*- 
ei==a'-b;from whence b=sa*e |-1 oate*-}-10 
a? 31-520", rejecting e* becaufe of its fmalnefs. 


Whence = = a’ @-\-2ae? -|-2.4e3--e*, and ad- 
ding on both fides ;2*,we fhall haveV tats ob 
ant f 5a* sennodigtt “\-220! “| e*==*4a-1ae-lee. 
Then fubftracting jaa from both fides, sate 


¥ Re arene eg 
bd Pale Se Vy 446 = ° é 
will 5 hale a 9 to which if: a be 


added, then will 4 e—%4 Fal pee p Petre 
eoehianns a bit signed, pox 
= the root of the Power 4‘+¥. But if it had 
a‘—b (the quantity 2 being too great ) the 
a Rule would have been thus,'4 Wa 6 --\4a. 
| | 54 
And this Rule approaches wonderfully, fo that 
there is hardly any need of Reftitution. — 
But while 1 confidered thefe things with 
my felf, I light upon a General Method for 
the Formulas of all Powers whatfoever, and 
(which being handfome and concife enough) 


- | } thoughtcI would not conceal from the Pub- 


lick. : pen "Thefe* 


fact bear or SNE 


Maite Cu wee a7 es 


4; hefe Formula’s, (as well the Rariowal,, as 


the Irrational eee) are thus. 


penne 


| ao 
Vv? a be ab Vee !a0— or 4-- oF ae ; 
. | 34aa--b 
OMe Vai ly == OF at 


fia" “+b = 3 4-|- Vs 16 aat- — re 

if Sars pee 4a+ Va A aa+ Treo 

“/74 pte’ 6 aa- iy ; ——;,ora}+_47__ 
Ia. 7A 


And fo alfo of the other a P 
if 2 were affumed bigger, than 


fought (which is done with fom advantage, 
as often as the Power to be Refolved, is much 
nearer, the Power of the zext Greater. whole 
“Number, than of the zexr lefs) in this cafe, — 
 Mutatis Mutandis, we shall have the fame Exe 
Pepons of the Roots, viz. 


NS POS ee Pe ie Bly Ae RN eR, peas: 
“ re 2 


2B | Mifcellanea Curiof 


é 


a—ih 


V aa Vaa-b, or 4—-—— 
24 

/' oped, or — a 
3a” Bk : 


Vv‘ tbrtat Vena! =! or am a 


% - ¥ pie h LAs | ab bs 


4 , amy 
tee! ae 104? 54° 2b 


ace ey : ab 


¢€ a 
4/ r fra ats 
V aka tal \ lr beet Mca 7 ae aj 


ri ‘ ‘ 
; “a b 


V a’—b = a-\- NV ikeaiel “hos of 4—- 
214? 


18; Tle ne 


ogg’ within: thefe two Terms, ‘thé true 

Root i is ever found, being fomething nearer 
to the Irrational than the Rational Expreffion. 
But the quantity e found by the frrarional For- 
muja, is always too great, as the Quotient re- 
fulting from the Rational Formula, is always 
too little.And confequently,if we have -|-b,the 
Irratioxal Formula gives the Root fomething 
greater thanit fhould be,and theXatioval fome- 
thing lefs. But contrary wife if it be—b. 


And 


Maifcelanea Curifa. 79 
And thus much may fuffice to be faid, con- 
cerning the extraction of the Roots of pure 
Powers; which notwithftanding, for common 
Ufes, may be had'much more eafily by the 
help of the Logarithms. But when a Root is 
to be determin’d very accurately, and the Lo-: 
garithmick Tables will not reach fo far, then’ 
we muft neceflarily have recourfe to thefe, or’ 
fuch like Methods. Farther; the Invention 
and Contemplation of thefe Formule, leading | 
me toa certain Univerfal Rule, for adfected. 
Equations (which I hope will be of ufe to all 
the Students in Algebra. and Geometry) I was. 
willing here to give fome account of this Dif- 
covery, which I will do with all the perfpe- 
cuity I can. I had given at N% 188 of the 
Tranfattions, a very eafy and general conftru- 
ction of all adfected Equations, not exceeding: 
the Biquadratick Power; from which time 
had a very great defire of of doing the fame in 
_ Numbers. But quickly after, Mr. Raphfon 
 Meem’d in great meafure to have fatisfy’d 
this Defire, till Mr. Lagvey by what he 
had perform’d in his Book, intimated that the. 
thing might be done more compendioufly yet. 
Now, my Method is thus. 
Let z the root of any Equation, be imagin’d 
to be compos’d of the parts 2+ or —e, of 
which, let 2 be affum’d as near z as is poffible; 
which is notwithftanding not zeceffary,but only 
commodious. Then from the Quantity a-+e or 
a—e, let there be form’d all the Powers of z, 
_ found in the Equation, and the Numerical 
Co-efficients be refpectively affix’d to them : 
-_ Then let the Power to be refolv’d, be fub- 
ftracted; from the fum of the given Parts ( il 


en et a ee a ee 
GY y Es wh Saas 
rc . a 


80. § MifceHanea Curiofa.” 


the firft Column where eis not found) which 
they call the Homogeneum Comparationis, and 
let the difference be +b. In the next. place, 
take the fumof all the Co-efficients of e in the 


fecond Column, towhich put=s. Laftly, in' 


the third Column let there be put down the 


fum of all the Co-efficients of ee, which fam. 


calle. Then will.the Root z ftand thus in 


; : : sb 
the Rational Formula, viz. 2 = a-|- 


and thus in the Irrational Formula, Vix. © 


sor) ORS Ae Vs ssE bt; which perhaps it 
ie ¢ 


m ; f t ‘ , 
may *be worth while to Iluftrate by fome 


Examples. And inftead of an Jnftrument, let 
this Table ferve, which fhews the Genefis of 


the feveral Powers of ate, and if need be,’ 


may eafily be continued farther, which for 


its ufe I may rightly call a General Analytical. 
Speculum. The forementioned Powers arifing” 


from a continual Multiplication by 4--e (=z) 


come out thus with their adjoyned Co-effici-— 
ents. See the Table. But now, if it be a—e=z,’ 
the Table is compos’d of the fame Members, - 


only the odd Powers of e, as ¢, ¢3, e?, e? are 
? 4 9 ») 


Negative, and the even Powers, aS e*, e4,e*, 


Affirmative. Alfo let the fum of the Co-efhi-’ 
cients of the fide e, be = 5; the'fum of the’ 
Co-efficients of the Square ce=¢t, the fum of: 


the Co-efficint of e* = u; of et = wm ,0fe=x, 


of e®=y,&c. But now, fince e is fuppofed™ 
only a fmall part of the Root that is to be en-— 


quir’d, all the Powers of e, will be much lefs 


than the correfpondent Powers of a, and fo far + 


the 


554th? 


2 


MifceHanea Curiofa. 81 


the firft Hypothefis; all the fuperior ones 
may be rejected ; and forming a new Equati- 
‘on, by fubftituting ate—z, we fhall have (as 
was faid) +-b—=se | tee. The following Ex- 


= 


~amples will make this more clear. 
Example I. 


_ Let the Equation z2!—3z?-| 75 z—=10000, 
be propos’d. For the firft Hypothefis, let 
=10, and fo we have this Equation, 


24==1a* yae tae? ae? \e* 
—dz2#——da af! ae—de* ‘ 
Tez—=|e2 ce | 
==T10c00 4000e |6o00ee 4oe? tet 

— 300  G60e —~ 3¢e 
Hyg FW): 738 
——10000 

4-450—- 40tge +597¢e—40e? -e’—=o 
APs Seme s t U . 

The Signs -- and — with refpe& to the 
Quantities e and e’, are left as Doubtful, till 
it be known whether e be Negative or Affir- 
mative ; which thing creates fome difficulty, 
fince that in Equations that have feveral 
Roots, the Homogenea Comparationis (as they 
term them) are oftentimes encreafed by the 
minute quantity 2, and on the contrary, thar 
‘being increafed, rhey are diminifhed. But the 
Sign of eis determin’d from the Sign of the 
Quantity 6. For taking away the Refolvend 
from the Homogeneal formed of a2; the Sign of 
se (and confequently of the prevailing Parts 
in the compolition of it) will always be con- 
Tt: G trary 


—y 


32 © ©Mifcellanea Curiofa, 
trary to the Sign of the difference 6, Whence 
"twill be plain, whether it muft be -| e, or —e 5 


and confequently whether a be taken greater 
or lefgthan the True Root. Now the quan- 


tity e is ==}s— Nf Benth when 6 and ¢ have the: 


t 
fame Sign, but when the Signs are diffe- 


Soe 


rent, e is = yet But after it is 


found that it will be! ~e, let the Powers e, e?, 
and e', @c. in the affirmative Members of 
the Equation be made Negative, and in the 
Negative be made Affirmative; that is, uf 
them be written with the contrary Sign. On 
the other hand, if it be +e (let thofe fore- 
mention’d Powers) be made Affirmative in the 
Affirmative, and Negative in the Negative 
Members of the Equation. 
~ Nowwe have in this Example of ours,1o450 
inftead of the Refolvend 10000, or b=+- 
whence it’s plain, that 4 istaken greater Ran 
theTruth,and confequently,that *tis—e. Hehe 
. the Equation comes to be, 10450—4o1§ e -|- 
§97ee—4e*-te* = 10000. That is, 450-4015 e 
b5o7ce 0; and fo 450 FA4OlS €—§97 € ey 


orb=se— tee, whofe Root ¢= oo V $s bt 
t 


or — Ag le that is in the 'prefent cafe, 
at Ph 5 i 2 


= ETSI 7514068 from whence we have 
597 

the Root fought, 9, $86, which is near the 

‘Truth. But then fubivting this. for,; a, fe- 

| cond 


Sy 
‘ 


Maifcellanea Curiofa. 83 
cond Suppofition, there comes 2t-e=z, moft 
accurately ap 8862603936495 . . fcarce ex- 


‘ceeding the Truth by 2 in the laft Figure, Uz. 
| bs Vases sobbe —isme. And this (if need be) 


may be An much Giri verified »by Be 
ing (ifit be+-e) the quantity aia 
from the Root before found 5 or (it it bee ) 


yei—te& 
by adding ot to that Root. Which 


v3 45S—t 
Compendium is fo much the more Valuable, 
in that fometimes from the firft Suppofition 


alone, but always from the fecond, a Man 


may continue the Calculus (keeping the fame 


Coefficients) as far as he pleafes. It may be 


noted, that the fore-mentioned Equation, has 
alfo a Negative Root, wz. z= 10,26. 
which any one that has a mind, may deter- 
min more accurately. 


Example II. 


Suppofe 1 1% $42 350, andletam 


fo. Then according to the prefcript of the 
Rule, 
rt o+2= 3 34° =rs ae -|-eF 
 adzis Eye ee 

dy speaeacat ge be 


G 2 . That 


= Wha ce ent eae 
1 7 daira 


84 Mifcellanea Curiofa. 


b t 
That is, -l-ro0o0t300e+30e? Fe? 

+1 900—-340e771 Je” 

+-540-+-§4¢ 

350 | 
OT. 5 LO —510 T14e nat 3ee 1 cele? = 0. Now, fince 
we have —510, it is plain, that 2 is aflumed 
Jefs than the Truth, and confequently that e 
is Affirmative. And from (the Equation ) 


s1O= 14e 24 Fe7 5 COMES € = V bets —Zz5 


t 
visa Whence z= 15,7..., which is 
too much, becaufe ef z taken wide; therefore 
Secondly, let a=15, and by the like way of 


Reafoning, we fhall find ex 2s— (Sib 


Lapeer reiaae ai 


¢t ‘ i 


I 
= — 2G08 hati “9 and confequently <= 


One 
14,954068. If the Operation were to be re- 
peated the third time, the Root will be found 
conformable to the Truth as far as the 25th 
Figure; but he that is contented with fewer, 
by writing tb te? iclatita of ¢6, or fubftra- 


Ging or adding ae or = sod EE the Root before 
found, will prefently obtain his end: Note, 
the Equation propofed, is not explicable by 
any other Root, becaufe the Refolvend 350s is 


greater than the @ube of = a 
«Example 


; he A te , af 
# 


MifceHanea Curiofa, 85. 
Example Mil. 


Let us takethe Equation z*—80 z5-1-1908 
27 149372 b50c0o=0, which Dr. Wallis 
ufes Cap. 62 of his Algebra, in the Refolution 
of a very difficult Arithmetical Problem where 
by Vieta’s Method he has obtain’d the root moft 
accurately;and Mr. Raph/oz brings it alfo as an 
Example of his Method, Page 25, 26.. Now 
this Equation is of the form, which may have 
feveral Affirmative Roots, and (which increa- 
fes the difficulty) the Coefficients are very great 


in refpect of the Refolvend given. 


But that it may be the eafier manag’d, 
let it be divided, and acccording to the 
known Rules of Posting, let —z*\ 823 - 
20 z? 15 z=0,5 (where the quantity zis ¥; 
of z in the Equation propofed) and for the 
firft Suppofition, let a= 1. Then |-’*— 5e— 
2e?-|-4e?—e4— 0,5 0 5 that is, 14= ge b2ee 5 
‘thence e= V3 sstbt — 3 is =37—5, and fo 


x» ¥ 


z=1,27;, Whence ’tis manifeft that 12,7 is 
near the true Root of the Equation propofed. 
Now Secondly, let us fuppofe ~=12,7, and 
then according to the directions of the Table 
of Powers, there arifes . 


b $ t u 
—=26014, 4641-8193, 532e—967, 74¢%7—-50, 8e3 — EF 
-\-16g870, 540-|-38709, 60e-+3048 ¢7%-|-30 @ 
322257, 42 —-50749, 2 e—1998 ¢? 
“189699,9 -|-14937, © 


mm 5900s 
7 G 3 That 


86 Mifcellanea Curiofa. 
That is, +298, 6559-5296 132e-+82, 26 e* 
\-29,2e?—e* =03; And fo —298, 6559=— 
§296, 132 ¢182, 26¢ee, whofe Root e (accord- 


ing to the Rule) = zs Byte comes tQ 


? 


i | +3 
2.648, 066—./6987686, 166022 


ap D ee 


| 825 2646 ee 
50§644080331....ee lefs than the Truth. But 
that it may be corrected, ’tis to be confider’d 


14 


: Fan 0000 20% we. as @ \ 
ne ue? --%e ) or’ 0026201 ulighedateoog; 
! a/ Liss bt 26 4.354.23% AER ICE Sal's 


i] 


\ 


pee 


ee / , 55--bt--tue*- te* or which is all one 


3 


ty a 
2.648, 066--4/6987685, 67496597577 -.+- 
9257126 J 
5 0§644179448074402 =e; whence atemz 
the Root is moft accurately 12, 75644179448 
074402... as Dr. Wallis found in the fore- 
mentioned Place; where it may be obferv’d, 
that the repetition of the Calculus does ever — 
triple the true Figures in the affumed a, 


I ayer ge Te 
3 ze 


tg mee bt apes 
quintuple; which is alfo commodioufly done 
by the Logarithms. But the other Correction 


t 


QD 


i 


which the fir ft correétion,or 


PA Se ey 


Maifcellanea Curiofa. 87 
_after the firft, does alfo double the number 
‘of Figures, fo that it renders the affumed al- 
together Seven-fold ; yet the firft Correction 
is abundantly fufficient for Arithmetical ufes, 
for the moft part. 

But as to what is faid concerning the num- 
ber of Places rightly taken in the Root, | 
would have underftood fo, that when a is but 
i part diftant from the true Root, then the 
Frit Figure is rightly affumed ; if it be within 
gb0 part,then the two firft Figures are rightly 
affumed ; if within 7...5 and then the three 
fir are fo; which confequently manag’d ac- 
cording to our Rule, do prefently become 
nine Figures. , 
' It remains now that I add fomething con- 
cerning our Rational Formula, viz. e=- : 


ss-rb 
which feems expeditious enough, and is not 
much Inferior to the former fince it will 
triple the given. Number of Places. Now 
having formed an Equation from a:te =x, as 
before, it will prefently appear, whether 2 be 
taken greater or lefs than the Truth ; fince 
se ought always to have a Sign contrary to 
the Sign of the difference of the Refolvend, 
and its Homogeneal produced from 4. Then 
fuppofing -\-b--se-|-2— tee =o, the Divifor is. 
ss—tb, as ofren as ¢ and b have the fame Signs; 
-but it is ss-\-bt, when they have different ones. 
But it feems moft commodious for Practice, to 


write the Theorem thus,e= ESN Keo fince 


this way the thing is done by one Maultiplica- 

tion and two Divifions,which otherwife would 

require three Multiplications, and one Divi- 
t : Z G 


cette 4 aun eet 


88 Maifcellanea Curtofa. 
Let us take now one Example of this Me- — 
thod, from the Root (of the foremention’d 
Equation) 12,7..-., where 
298, 6559—.§296, 132-182, 26¢ee129, 
“+b is i ae 


peel Sale 
2e3 —e* =0, and fi nT tae ees that is, let 


it\be as s tot, fo b to ah §296,1 32)2.98, 
S 


 6§§9 into 82,26 (4,63875..- wherefore the 


Divifor is s—- —. = 5291549325 ae ..) 298, 
5 as 
6559 (0, O§6441.-... e, that is, to five true 


Figures, added to the Root that was taken. 
But this Formula cannot be corrected, as the 
foregoing Jrrational one was; and fo if more 
Figures of the Root are defired, ’tis the beft 
to make a new Suppofition, and repeat the 
Calculus again: And then a new Quotient, 
tripling the known Figures of the Root, will 
abundantly fatisfie even the moft Scrupulous. 


A Differe 


Mifcellanea Curiofa. $9 


A Differtation concerning the Con- 
- firuction of Solid Problems, or 
Equations of the third or fourth 
Power, by the help of one (given) 
Parabola and a Circle. iit: 
: By Edmund Halley. 


¥ YOw all Equations (that involve the third 
or fourth Power.of the unknown Quan- 
tity) may be conftructed by the help of any 
given Parabola and a Circle, the Famous M. 
Des Cartes has fhewn and clearly demonftrated 
in the Third Book of his Geometry. But he 
firft of all orders the fecond Term of the E- 
' quation (if it be there) to be thrown out, and 
then by the Rule there delivered, to find the 
Roots of the Equation fo reduced. 
‘ And fince that Operation feems too La- 
borious, fome thought fit to invent a like 
Conftruction, without any previous Reduttion. 


_- Amongft whom Frazcis a Schooten has offer’d a 


Method (for conftructing cubical Equations 
-howfoever affected) which might have been 
called very eafie and fimple; if (by unfold- 
ing the Principle from whence he deduced his 
Rule) he‘ had better confulted his Reader’s — 
Memory, which he burdens with very many 
and perplex’d Cautions. But lately our Fa- 
mous Countriman, Mr. Thomas Baker, in a 
whole Treatife written upon thefe Conftru- 
3 oe | | étions, 


go me Mifcellanea Cuntafa. co! 


tions, has comprehended not.only all Cubi- 
_ cal, but alfo Biquadratical Equations of every 
kind, under one General Rule, which he has 
~ demonftrated, and abundantly Iiluftrated with 
Examples through ail Cafes; and moreover 
at the Clofe, propos’d a way, by which that 
Gencral Rule might be Invefligated. But he 
does not fhew the very Method, by. the-help 
of which (as I fufpect) he obtain’d his Umi- 
ver {al Geometrical Clavis, or at leaft might have 
obtain’d it with much more eafe. And fince 
this Rule of Baker’s is no lefs perplex’d with 
Cautions about the Signs +> and — than Schoo- 
ten’s is, fo that a Perfon can hardly perform 
thofe Conftructions aright, without he has the 
Book by him; I thought that it wou’d not be 
either Unpleafant or Unprofitable to young 
Students, to. explain the Foundations of both 

Rules, and by fome emendation of the Me- | 
thod once more, to afford as much light as I 
coud in fo dificult a Matter. Cartefius's Con- 
ftruction (which does very eafily difcover the 
Roots of all Cubick or Biquadratick Equati- 
- ons, where the fecond Term is wanting) may 
be fuppos’d as known. Yet fince ’tis the main 
bottom, on which all that follows does de- 
pend ; that this Diflertation may not feem to 
want a principal Part, I'll here add the Rule 
taken out of his Geometry, altering fome few 
things (as I think) for the better. 
- The fecond Term being out of the Equati- 

on; all cubical Equations, are reduced to | 

this Form, z’y. apz. aaqeo3 and Biquadra- - 
tical ones to this Form, <*. y. apzz. aaqz. 
a*r =o, where a.denotes the Latus Rectum of 
any given Parabola, which, is ufed ~ the 
one 


Mifcellanea Curiofa. 91 
ConftruGtion. Or elfe- taking @ for Unity, 
thofe Equations are reduced to thefe Forms, 
viz. Cub. z3. yp x. g =0,and Biquadr. z*y.pzz, 
qz.r.=t 0. Now the Parabola FAG, Fig. 9 be- 
ing given, whofe Axis is ACDKI, and Para~ 
meter= zort; let AC be taken= 2 4, and 
be fet off always from the Vertex _4, towards 

_ the inner parts of the Figure. Then take CD 
2 p, in that Line AC, continued towards C, if 
it be ---p in the Equation, or towards the 
contrary Point, if it be tp. Farther,from the 

point D (or from the point C, if the quantity 

_ pbe not in the Equation) Let DE (erected 
perpendicular to the Axis) be made= 2g 
which is to be fet to the right hand if it be 
---g, but to the other fide of the Axis if it be 
--g. And then a Circle defcribed on the 
Center E, which the Radius AE (if the Equa- 
tion be but a Cubical one)-will interfe@ the 
Parabola in as, many Points (viz. F, G, G,) as 
the Equation has True Roots, of which the 
Affirmative ones, as GK, fhall on the right 
fide of the Axis, and the Negative ones as 
FL, on the Left. But if the Equation be a 
Biquadratical one, then the Radius of the Cir- 
cle AB, by adding (if it be ---7) or Subftraa- 
ing (if it be -v) from the Square of it, the 
Re@-angle 4 «7, or the content under the. Pa- 
rameter, and the given Quantityr; which is. 
very eafily done Geometrically. And the In- 
terfections of this Circle with the Parabola, 
will give (letting fall Perpendiculars from 
thence tothe Axis) all the trve Roots of 
the Biquadratical Equation; the Afirma. 

- tive ones being on the Right fide of the Axis, 
‘and the Negative ones, on the Left. The de. 

ie eS arcs demon- 


92 Mifcelanea Curiofa. 


monftration of all which I leave to Cartefius 
‘the Inventor. Let it be Noted, that I endea- 
vour here that the Affirmative Roots, may 
always be had on the Right fide of the Axis, 
to avoid the Confufion that will neceflarily 
arife from a multitude of Cautions, where the 
reafon of them is not evident. 

Having premifed thefe things, in order to 
make way for the conftruction of thefe Equa- 
tions, even when the fecond Term is found 
in them, we are to confider the Rule it felf 
for taking away the fecond Term, and redu- 
cing the Equation to another, fuch as might 
be conftruéted by the foregoing Method. Now 
all Cubick Equations of this Claffis, are re- 
duced to this form, z* 6zz. apz. aaq =o, or to 
this, 2%. bz”. y. aaqgz=o. Biquadratick onés 
may be reduc’d to this, 2*. bz. apz*. aaqz. 

a’r=o, or this, z*. or this z*. 623.4. aagz. 
areio, or this, z*. bz3. apz?. x. air mio, Or 
laftly, to this Form, z*.bz5 y. y. @r=o, 
From all which there arifes a great Variety, 
according as the Signs + or — are diverfly 
connected, together ; and hence the General 
Rule ferving all thefe cafes, is rendred very 
obfcure and difficult, unlefs (manag’d by the 
help of the following Method) it be cleared 
up and delivered from thofe Intricacies. _ 

The fecond Term in Biquadratical Equati- 
ons, is taken away by putting «=zT Jb, if it ~ 
be -+d in the Equation; or «=z—7), if it be 
—b. Hence x; 6 in the firft cafe, and x. 
+b in the fecond, is = 3 and fo in any Equa-~ 
tion propofed, fubftituting inftead of z, its 
Equal, there will come forth a new Equation, | 
wanting the fecond Term, all whofe ik 


— Mifcellanea Currofa. 92 
do exceed, or come fhort of the fought’ Root 
z, by the given difference 44. But fince in 
things of this kind, Examples do more than 
Precepts, let us propofe one or two Equati- 


- Ons to be conftructed. 


E xample Is 


uA+-b23 —aprz---aagqz aire. 

put x---56=7, and then will 

Mame be H- bb 2. 

HF want 7b + 2.xb* --- 2,55 = 23. and 
mn x3-+ 2 O x2~0- 2b) x 1,264 =. 2* 


Hence it follows, that 


xt eb 2b2x2 --- 3 bix + i4.b4 ~*, 
bx3---3.b? x? -| 3 b3 x--- Ab = 1bz3 
=--apx? |S apbec---shapb” rm ---apz” 
en-au ia’ qb —a*qz 
Tair 


The Sum of all thefe is a new Equation 
wanting the fecond Term, and which confe- 
quently may be conftructed by Cartes’s Rule, 
by taking inftead of 5 p, half the Coefficient 
of the third Term, divided by 4 or the Para- 


ae b é 
meter, that is—,3 2 2p; and inftead of 3g, 


half the Coefficient of the fourth Term, divi- 


ia : Aah ee . pb 
ded by aa, that is, Fas a i ae The 


Mem- 


94 Mifcellanea Curiofa. | 

Members of which that have the Sign -|- are 
to be fet off to the left Hand from the Axis, 
and thofe that have the Sign to the Right 5 


in order to find the Center of the Circle re- © 


quired for Conftruction, whofe Interfections 
with the Parabola (letting fall perpendiculars 
to the Axis) may give all the true Roots ~, 
namely, the Affirmative ones on the Right 
fide of the Axis, and the Negative ones on 
the Left. But now, whenwx— b= 2%, then 
drawing a Line Parallel to the Axis on the 
right fide of it, and at the diftance of =), the 
Perpendicularg terminated on this Parallel, 
will denote-all the enquired Roots z, the Af- 
firmative ones on the right fide, and the Ne- 
gative ones on the Left. As for what relates 
to the Radius of the Circle, it is had, by ad- 
ding the Negative, or taking away the Af- 
firmative parts of the fifth Term divided by 
aa, from the Square of the Line AE, drawn 
from the Center E found, to_4 the Vortex of 
the Parabola; which is moftly done, by ta- 


king iuftead of AE, the Line EO which is — 
terminated at O the Interfe€tion of the Para- 


bola, and the fore-mentioned Parallel; for the 
Square of this comprehends all the parts of 
. the fifth Term, brought into the new Equa- 
tion upon the cafting out of the fecond Term, 
.asis eafily proved: And it remains only, that 
the square of EO be increafed, if it be. ---7, 
in the Equation, or diminifh’d, if it be “Ir, by 
the addition or fubftraction of the Rettangle 
ar from whence the Radius of the Circle de- 
fired, is compos’d. This Method of inveftiga= 
ting M. Baker’s central Rule, is eafie and free 
#romvall Cautions; and the difference arifes oe 

y 


ee wee eT oie 
r4 8 ‘ 
7 


Mifcellanea Curiofa. 95 

ly from hence,that J determin the center of the 
Circle, by the Axis, and he by a Parallel to the 
Axis, and that 1 always have four Affirmative 
Roots on the right fide the Axis, which hehas fome= 
times on the right fide, and fometimes on the left. 
' As for cubical Equations, they are to be 
reduc’d to Biquadratical ones, before they can 
be conftructed by the fame General Rule; 
which is done by multiplying the Equation 
proposd by its Root z; whence arifes a Bi- 
quadratick Equation, in which the laft Term 
or r, is Wanting. Wherefore taking away the 
fecond Term, and finding the Center E, the 
line EO isthe Radius of the Circle; viz, 
When 47 is =o, and the whole fifth Term 
in the new Equation, arifes from the taking 
away ofthe fecond Term. Let this Equation 
be propos‘ to be conftructed. 


Example if. 


Z3 = bz* -bapz Faaq= o, 
which multiply’d into z, becomes 
OR CAPS | BAGS EO. 
To take away the fecond Term, put 
Kbeg OS z, and then will 
xt Chek 7 4 bb? bin 1552 b* me +4 
— bx? 4 baxter Bb J bem bs 
reaps? 1 2 abpx|\1,apb? eat “apes 
‘bh aaqxe\)aagb = Vaagqz. 


"Now in this new Equation, the half Coef- 
ficient (of the third Term) divided by 4, wz. 
my a |-2 p, is to be ufed inftead of z P} and 


Le by adiad “at 2 bale eal, Mahi 


96 Mifcellanea Curiofa. 


the half Coefficient of the (fourth Tertn) di- 
vided by a a, the Square of the Latus Rettum, 
| b 


4 


pe 29, is inftead of 34 in 


Vi%Z. i 
16a* 

‘Cartefius’s Conftruction, from whence the Cen- 
ter Eis determind. Then drawing a Paral- 
lel to the Axis, at the diftance £4, to the left 


fide (becaufe of y= « 1-15) whofe Interfecti-. 


on with the Parabola, let be O; a Circle de- 
fcribed on the Center E with the Radius EO, 
will cut or touch the Parabola in as many 
Points as the Equation has true Roots, which 
Roots,or z,are the Perpendiculars let fall from 
thofe Points upon the Parallel to the Axis, 
the Affirmative ones to the Right fide, and 
the Negatives to the Left. Ifthe third or 
fourth Term,or both, be wanting in the Equa- 
tion, there’s no difference at all ( of the Me- 
. thod of inveftigating the Central Rule) to be 
obferv’d. But the Quantity p or g being want- 
ing, thofe parts.of the Lines CD and DE (in 
fome manner deduced from that Quantity 

will be wanting too, and we are to procee 


with the other Coefficients of the third and 
fourth Term in the new Equation, according — 


to the way prefcrib’d in the foregoing Exam- 
- ples. 


Hitherto we have confider’d Mr. Baker’s 


General Method, than which none more Eafie 
and Expeditious ts to be expected, ufing either 
a Parabola, or any other Curve for a Conftru- 
ction, viz. when the Equation rifes to the Bi- 
guadratick Power. For while I am writing 
of this, ’tis my good Luck to hit upon a cer- 
tain Geometrick, Effection of the central Rule, 
which is Expeditious beyond Hope, and will 


abun- — 


EE 


; 2) Curiofa. 97 

‘abundantly fatisfy thofe that are curidus in 
thefe Matters. | 

(Fig. 10.). Having defcrib’d the Parabola 

NAM, whofe Vertex is 4, Axis ABC, and Pa- 

rameter 4; let the Fquation be reduced to this 
Form, zt. bz}. apz*.. aaqz. a?r. == 03 or 

if it be only a Cubical one, to this, z}. gen 
‘@pz. aaq. = o. Then at the diftance BD 4), 
Jet DH be drawn parallel to the Axis (to the 
Left Hand if it be—4, and. to the Right, if 
it bed) meeting the ‘Parabola in the point 
D, from whence let fall BD. perpendicular 
to the Axis. In the Line AB continued to- 
wards B, make B K==;4, and draw the Line 
DK. interminate on either fide: < Harther, 
take K C==2 AB, always in the Axis produ- 
ced beyond K; and if the quantity p has 
the ‘Sign =i, take towards the fame parts, 
CE", but towards the contrary part, if 
it be tp. Then at the point E (but at the 

point C if the quantity be wanting) erect 
EF. perpendicular to the Axis, meeting Cif . 
need be) the-Line DK prodtced, in "the 
point F, which point is the Center of the 
Circle required, if the quantity g be want- 
ing. But if g be in the Equation, then we 
muft take in the Line F E (if need be) pro- - 
duced the length of F G==34, which place 
to the Left Hand if it beg, but to the 
Right if it be —q; and then the point G 
wil ll be the Center of the Circle required for 
the Conftruétion, and the Radius of it, will 
be the Line GD, if the quantity + be want- 
ing, that is, if the Equation be only a Cubi- 
‘al One; the Square of which fame Line (in 
Bididdiatick pingsens) is to be i 
¥ 


Harare nme PRTC ORCEN Se er 


98 Mifcellanea Curiofa. 

by the addition of the Rectangle under + 
and the Latus Rectum, if it be —r, or to 
be diminifhed by the fame Rectangle if it be 
-+-r. The Circle thus deferib’d, and Perpen- 
diculars let fall from its InterfeGtions with 
the Parabola, to the Line DH, thofe that 
are at the Left Hand as NO will always be 
the Negative Roots of the Equation, and 
thofe at the Right, the Afhrmative. 

Cubick Equations are otherwife (and fome- 
thing more fimply) conftruéted according to 
Schooten’s Rule, m which alfo the Roots re- 
fpe&t the Axis. But becaufe the Inventor 
himfelf does neither explain the Inveftiga- 
tion nor Demonttration, it will not be amifs 
to fhew the Foundation of it here, and at 
the fame time render the Geometrick Con- 
itruion more Elegant, and rid it of thofe 
Cautions in which ’tis involw’d. 

This Rule is deriv’d from hence, that 
every Cubick Equation may be reduced to 
a Biquadratick one, in which the fecond 
‘Term is wanting. Which is done, by mul- 
tiplying the Equation propofed into z —bme, 
if it be 1b in the Equation, or into z--b=0, 
if it be -b; and the new Equation thus 
form’d will have the fame Roots with the 
Cubical one, and moreover another Equal to 
+b, if it be —b in the Equation, or con- 
trariwife. © 

Let the Equation z<? +2’ b--apz ---aag=0, 
be propofed to be conftruéted ; multiply this. 
inte <-+b, and it makes. 

x mt 23D-\-apz*-|-aaqZ, 
4-23 b—bbz’-|-abpz--aagb . 
| Here now the fecond Term is wanting, Ai 
the 


+ WMifceHanea Curifa. — 99 
the Coefficient of the third Term — bb-\-ap, 
gives os id 4-2 p, in the room of 3p or CD 


in Cartefiuss Conftruction; and from half 
the Coefficient of the fourth Term is made — 
&g-- iB, inftead of 3q or DE, and fo the . 
Center of the Circle fought is determin’d. 
Alfo becaufe one of the Roots of the new 
Equation, vz. -\-b is given, a point in the 
Circumference will’ be given too, and confe- 
quently the Radius. | Laftly, Having de-. 
icrib’d the Circle, Perpendiculars let fall 
from its Interfections with the Parabola,- to 
the Axis, will give the Roots of the Equa- 
tion, both Affirmative and Negative, in the 
Jame manner as before. : 
_ Now the Center of the Circle is found by 
a moft eafy Conftrudction, and which is to be 
preferr’d to all others, in Cubick Equati- 
ons. 

_ Fig. 11. Let 4 be the Vertex, arid AF the 
Axis. of the deferib’d Parabola AMD; at a 
diftance equal to 6 let DK be drawn parallel — 
to the Axis, to the Right Hand if it be-|-6 
in the Equation, and to the Left, if it be 
—b:; which Line fuppofe to meet the Para- 
bola in the point D. Upon the Centers D 
and A, and with equal Radij, defcribe on 
both fides two occult Arches, interfecting 
One-another, and thro’ thofe points of In- 
terfeGiion draw the interminate Line BC 
which cuts the imaginary Line AD in the 
middle and at right Angles, and meets the 

| H 2 : Axis 


- 


A eee eh Gy i i'w 
mS BPs bin, DECC, Ue TORT aes = 
PAR i ha Ae rer y sui 


1900) Mafcellanea Curiofa. 

‘Axis in E. From £ fet off EF = 3 p, down- 
wards, if it be —p in the Equation, but up- 
_ wards towards 4 if it be +p, then at the 
| point F(or £, if p be wanting) erect the Per- 
-pendicular F G, meeting the Line BC in G, 
and in GF produced take GH = 34, to the 
Right Hand, if it be ~q in the Equation, 
but to the: Left, if--g.. Then will the point 
#1 be the Center, and HD the Radius of the 
Circle fought, which (¢letting fall Perpendi- 
culars to the Axis from its Interfections with 
the Parabola) will fhew all the Roots (as 
LM) of the Equation. And how this Con- 
ftrudion follows from what went before, is 
evident enough of it felf, fo that there is no 
need of infifting any farther upon the De- 
monftration of it. | : 


! 


A Dif 


“ 
4 
= ‘ 
aay 
‘ 
ope) ‘ 
~ ‘ Uy 
x 
. ‘ zs +e ’ 
. My “ ts 
py) ae ~ 
ae ae 
BN aes oot See = = = 
& “S mae 
é ato Noe So» 
: z > Fig d . 
at x 
ee \ 
4 ’ 
‘ 
‘ ‘ 
a N 
‘ 
’ 
' 
' 
. ‘ 
F i 
‘ 
‘ 
‘ 
, 
4 
4 
‘ 
4 
4 
; 2 iz 
se . 
= = 
fe 


jal aa 


eae ee 


Mifcelanea Curiofa. 101 


LY 


i 4 


A Difcourfe concerning the Num- 
ber of Roots, i Solid and Bi- 
quadratical Equations, as alfo of 
the Limits of them. : 

| | By E. Halley. 


| HY in the precedent Difcourfe fhewn 
a Method, by which folid Problems 
however affected, might be conftruéted after 
‘a moft fimple and eafy manner, by the help 
_of one given Parabola and a Circle ; towards 
the latter end a certain pleafant Speculation 
‘offer’d it felf, namely, that from thefe Con- 
_ftrudctions, the Number of Roots in any E- 
quation, with their Limits and Sines, would 
eafily follow and be determin’d. Upon which 
‘account, I promis’d that I would quickly 
‘write a fhort Differtation concerning this 
Subject, in which I was perfwaded I fhould 
perform fomething not unprofitable nor un- 
‘grateful (if not to the Geometers of the 
firft, yet at leaft) to thofe of the fecond 
Rank. sence He Bi 
. But coming to look nearer into the Bufi- 
nefs, I found I was imprudently fallen in 
among fome of the profound Difficulties of 
Geometry, and deftin’d to handle the fame 
Things, that formerly .employ’d the Pains 
of two Tluftrious eet apate and Cartes 5 
‘Gabi colonel 3 il 


102 Maufcellanea Curiofa. 
in which they either of them (by a like Fate 
tho’ in a different way) committed a Para- 
logifm, perhaps the only one in all their 
Geometrical Writings ; as fhall be afterwards 
prov’d. Wherefore being fenfible, as well of 
the Difficulty, as the Excellency of the Sub- 
je&t, I refolv’d to apply to it ftrenuoufly, 
that I might not be thought unable to per- 
form my Promifes, and that fo noble part of 
Geometry, and fo little cultivated, might 
not lie any longer wrapt up in Darknefs, but 
‘be render’d plain and intelligible by thefe 
few Lucubrations of mine. But firft the 
Reader muft take notice, that while he fets 
“to the. Reading of this, he ought to have 
“the foremention’d Differtation (Ao. 188.) at 
‘hand by. him, and to underftand the Con- 
ftructions there delivered very well; becaufe 
thofe things that follow do chiefly depend 
upon them, neither are they to be here re- 
“peated again. oan) | 
It is plain from Cartefivs, and what was 
there faid, that both in Cubick and Biqua- 
dratick Equations, the Roots may be expoun- 
ded by Perpendiculars let fall, upon the-Axis 
or. given Diameter. of the given Parabola, 
‘from the Interfections of that Curve with a 
Circle. And. whereas when. a Circle inter- 
teas a_Parabola, it muftneceflarily, do fo, 
“either in four or in two points; it’s manifeft, 
that in. Biguadraticks there, muttalways be, 
- Wegatives as alfo if the Circle happens to 
touch it, in which cafe the equality of two 
Roots.of the /ame Sign, is concluded, , But 
in Gubick, Equations, becaufe,pne,of the In- 
¢ Te ae terfections 


Mifcellanea Curiofa. 103 
‘terfections is requir’d to the Conftrudtion, 
therefore either but one, or the three re- 

maining Roots, do denote one or three; as 
in the cafe of Contact; whence its plain, 
that there are found two equal Roots, and 
that the Problem from whence the Equation 
refults, is realy Plaii. 
Therefore all Cubick Equations however af- 
fected, are explicable by one, or by three 
Roots, which are always poffible, that is, if 
we admit Negative Roots for trve ones. So 
Biquadraticks whofe laft Term 7 is affected 
with the Sign —, are explicable by two or 
four ; but if it be +-r in the Equation, and 


it be fo great that VGD q — ar (See Fig..10.) 
be lefs than that the Circle defcrib’d with 
- that Radius and on the Center G, can touch 
the Parabole in any point; the given Equa- 
tion is altogether impoflible, nor is it expli- 
cable by any Affirmative or Negative Root; 
but more of this in the following Pages. 
Now fince there js fo great a difference be- 
tween the Cafes of Cubick and Biquadratick 
Equations, that they cannot be comprehend- 
ed together, we will firft of all handle the 
-Cubicks, and then the others. ‘The Cubicks 
are conftruéted by an infinite Number of 
Circles in a given Parabola; but the Biqua- 
draticks by one alone (at leaft by thefe 
_ Methods) and that becaufe, putting z---e (or 
-any Indeterminate) equal to. nothing, the 
Cubick Equation is reduced to a Biqudratick 
having the fame Roots with the Cubick, and 
befides that, another Root equal to ¢; whence 
it comes to pafs that the Cubick Equation 
4 H 4. may 


mer aii 9 Seta Lk | 
i04 Maifcellanea Curiofa. 
may be conftructed by as many different Cir- 
cles, as you can imagine Quantities e, that 
is, an infinite Number. But among all thefe, 
_ that which I gave before, is the eafieft: Yet 
there is another not much inferior to this, 
which feems better accommodated to the de-’ 
figns of determining the Number of the 
Roots, and their Limits; and which arifes 
from the taking away of the fecond Term, 
by putting after the common way «=z 
-or — } of the Coefficient of the fecond 
Term. Now this way is thus: The Parabola 
ABY (Fig. 12.) being given, whofe Vertex. is 
A, its Axis AB, and Larus Refum a, \et the 
Equation be reduced to the ufual Form, vz. 
z3. bz. apz. aaq. to. ‘Then at the diftance 
of ; 4 let there be drawn BK (parallel to 
the Axis, to the Right Hand if it -- 4, other- 
wife to the Left) which meets the Parabola 
in B; and let the Line DP interminate on 
both fides, be ereéted perpendicular to the 
fuppos’d Line AB, meeting the Axis in the 
point G. From the point B, let fall the 
Perpendicular BC, and let GE be always made 
equal to AC, and be fet off towards the 
lower parts. From E fet off EH = 2 p, up- 
wards if it be ++ p in the Equation, but 
downwards if = p; and from the point A, 
(or E, if the quantity p be wanting) let the 
Perpendicular HQ be drawn out, méeting 
the interminate Line DP in O. Laftly, in 
the interminate Line HQ, make OR = ¢ 4, 
from O to the Right Hand, if it:be’— 4, but 
to the Left, if--g. Then a Circle defcrib’d 
on the Center R with the Radius RA, will 
cut the Parapola in as many points, as. the 
pes Tee © ~ Equation 


4 


— Maifcellanea Curiofa. 105 
Equation propos’d has Roots, and they will 
be the Perpendiculars ZY, let fall from the 
Interfections Y, to the Line BK parallel to | 
the Axis; of which thofe that are to the 
Right Hand of the Line BK, are the Affr- 
‘mative ones, and thofe to the Left, the Ne- 
gative. : Bee 
_ . The conveniency of this Conftruction, lies 
in this, that ’tis perform’d by a Circle paf- 
fing thro’ the Vertex, in the fame manner as 
if the fecond Term had been wanting. And 
therefore to determine the Number of the 
Roots, ’tis fufficient to know the Properties 
of the Place, or that Curve Line which di- 
ftinguifhes the Spaces, in which if the Cen- © 
ter of the Circle (that pafles thro’ the Ver- 
tex of the Parabola) be placed, the Circum- 
fetéhce of it fhall interfeét the Parabola ei- 
ther in one or in three other points: That is, 
to define the Nature of that Curve, in which, 
fall the Centers of all the Circles pafling 
_ thro’ the Vertex, and then touching the Pa- 
-rabola. Now this Locus, is that very Para- 
boloid, which the celebrated Dr. Wailis calls 
the Semzcubical, in which the Cubes of the 
Ordinates are as the Squares of the corre- 
fpondent Abfcifles, The Latus. Rettum of 
which, is #3 of the Latus Rettum of the gi- 
yen Parabola, and its Vertex the point U 
(Fig. 12.) the Line AU being half the Latus 
_Rettum of the fame Parabola. That is, if 
we put unity for the Latus Reétum of the gi- 
ven: Parabola, then 3; of the Cube of the 
ordinate applicate, will = the Square of the 
‘intercepted Diameter; or the Cube of 3 
YH =the Square of AR, wiz. if R be the 
dil Center 


106 Mafcellanea Curiofa. 
Center of the Circle that pafles thro’ the 
Vertex of the Parabola, and touches the fame 
afterwards. : if 
_ This is that Curve which our Country- 
man Mr. Ne (the firft of all Mortals) de- 
-monftrated to be equal toa given right Line, 
and by that means obtain’d a Reputation 
among the principal Geometricians. Its pro- 
perties have been curioufly enquired into, by 
Dr. Wallis, (at the end of his Book of the 
Ciffoid ) and Flugenius (Prop. 8 & g. of his 
Tra&t of the Evolution of Curve Lines) and 
others, whofe Writings the Reader may con- 
fult. This Curve defcrib’d on either fide of 
_-the Axis of the Parabola (viz. VNL, YPX) 
-comprehends a Space, in which if the Cen- 
ter of the Circle (which pafles thro’ the Ver- 
tex A) be placed, it will cut the Parabola in 
thnee other points. But the Spaces more re- 
mote from the Axis, do afford Centers for 
Circles that will cut the Parabola but in one 
-point befides the Vertex. e 
‘Thefe things well underftood, we are now 
prepar’d to determine the Number of the 
Roots. And firft of all, let the fecond Term 
be wanting, and let the Latus Rettum = 1, or 
AV =. Inthe Conftrudion VH is= 2p, HR > 
-r3q3 and fince if it be-+-p in the Equation, © 
zp is to be fet off from U towards the upper 
parts, the Center of the Circle is always 
found without the Space LVX, and therefore 
is explicable by one Root only, which is Af- 
firmative if it-he 49, Negative if --9 5 and 
thefe Roots’ may be inveftigated by Cardan’s 
Rules. But-if it be — p, then UH= 4p, is 
fet off towards the lower parts; and it is 
a3 poffible . 


F) RET MAR OS SET sy eae Sm) 
ee 4 i 


— Mifceilanea Curwfa. 107 
poflible that HR may fall between the Axis and 
the Curve UX or UL, wiz. if the Cube of 2 
UH or of p, be greater than the Square of 3 93 
that is, if z-p* be greater than 39°; in which 
‘cafe there are three Roots, two Negative, if 
it be — g, and one Affirmative equal to the 

fum of the others; but if it be +4, then 
there are two Affirmative ones, and one 
Negative. But if 2>p? be lefS than 3 97, 
_ then there is but one Root, Affirmative if it 
_ be 4, Negative, if -|-g. Allwhich things 
are taught by thofe that have handled this 
part of Geometry. | 
Now let all the Terms be in, and firft let 
there be propofed, as an Example, this Equa- 
tion, z* — 2” b\-zp-q =, to which Fig.12. 
ferves. In-the Conftruction of this, we have 
BCH:b, UGas AC 3’, VES yO’, 
 UH=26* 4317p, GH=36 tp, orip | 
36°. Hence HO= i, b? 4 45, or Shp me 
27 6*, and HR (that is the diftance of the Cen- 
ter of the Circle R from the Axis) is ever the 
difference between 3 bp and ,', b* +2 4,which 
Expreflions if they are equal, then the Center 
falls in the Axis: If 2 bp be greater than ;, b° 
+49, then it falls.to the Left Hand of the 
Axis, if lefs, then to the Right. If therefore 
the {quare Root of the Cube of 4 UH (that is 
of 3 6? 1p, or putting 5 67— ppd, 
if /ddd) be greater than HR, that is the 
difference between ,7 0' 39 and 2 bp; the 
- Genter R will be found within the Space — 
NPU circumfcrib’d by the Paraboloids UPX, 
UNL, and the interminate right Line DNP; 
and fo the Circle will cut the Parabola in 
three points Y, Y, Y, pofited to the Right 
Hand 


BA Ai 


108 = Mie sane’ Curiofa 


Hand of the Line BK, and fo the Equation will 
have three Roots. But the Center being with- 
out this Space NUP, it is explicable but by 
one Affirmative Root. ‘Here it may be noted — 
by the by, that the Right Line DP may touch 
the Paraboloid UPX in the point P, EP be- — 
ing #, 6? ; but will cut the other Paraboloid 
UNL in the point NV, fo that letting fall NF 
perpendicular to the Axis, UR ist \ EUs or - 
3407, and NF yo¢ 0%. But UW (which be- 
ing perpendicularly applied to the: Axis at 
the point UV; meets DP-in W) is = 4 b>, or - 
7 EP? 
* Hence we may 4 fafely conclude, that if-in 
the Equation either p be greater than $67, _ 
or gq greater than ,, 6%, that there will he | 
found but one Root, and that an Affirmative 
one. Carte’s Rule therefore (Page 70. Edit. 
Amftera. 1659.) is net true, in which he de- 
termines that there are always as many true 
Roots, as there are changes of the Sines +- 
and — in the Equation: Schooten in his Com- 
mentaries vainly endeavouring the defence 
‘of this’ Miftake. Alfo Prop. 5. Sect 5 OF 
our Country-man Aarriot’s Ars Analytice (as 
alfo Prob. 18. of Vieta’s Numer. Poteft. Retol.) 
is hardly found; fince from the Limitations 
- which they have there fet down, that muft 
agree to the whole Parallelogram PIUW,. 
which we ‘have prov’d does agree .only to- 
the Space NUP; that is to afford a Center 
to the Circle interfecting the Parabola in 
three other points befides the Vertex. 
But the quantity q or the laft: Term @ 
and P peut Sar fo that ? be pers 


—Mifeellanea Curwfa. 0g 
3 6?) is exadly limitted from the foregoing 
Equation Vddd= 3b +iqné bp; viz 
when the Circle touches the Parabola. There- 
fore; q ought to be lefS than ¢4p 37,07 
Va} ; but if p be greater than 407, alfo; 4 
ought to be bigger than ¢ bp 4 27 6? a a/d?, 
that the Center may not fall in the little 
Space NUW. And with thefe Conditions 
the Equation will always be explicable by 
three Roots; otherwife but by one. But 
whether there be three or one, they are al- 
ways Affirmative ones, becaufe of the pofi- 
-tion of the Center R to the Right Hand of 
the Line DP. | ie 
_ And this is the moft difficult Cafe; fo that 
thofe that well underftand what has gone be- 
fore, will without any trouble take what 
comes after. Now let the-Equation 2? —é | 
xz? pz qo, be given. Here (that there 
may be three Roots had) the Center of the 
Circle ought to be found fomewhere within 
the Space PNa, determin’d by the right 
Lines PN, Pa, and the Curve of the Para- 
bola Na; wherefore fince EF is= 3 00, p 
ought to be lefs than 4 4b. Now for the de- 
termination of the quantity 7, ¢ being = % 
b? 3p as before, /d? +27 6? — % bp ought 
always to be greater than} 9, that fo the 
 €enter of the Circle may be pofited in the 
forementioned Space PNa; which when ’tis 


fo, fuch an Equation has two Affirmative 


Roots, and one Negative. But if p be greater 
than } bb, or 39 greater than /d’ -l- 27% = 
é op; it is explicable but by one (and that a 
Negative) Root, Let 

Let 


FIO Maifcellanea Curtofa. 

Let the Equation 23 mbz? —pz—qma, be 
propofed in the next place. That this Equati- 
on may have three Roots, the Center of thé 
Circle muft be found fomewhere in the inde- 
finite Space between the right Line DPD 
and the Curve of the Paraboloid PX. The 
quantity p is not here liable to Limitations ; 
but 3 7 ought always to be lefS than /a? — 
z7 6? — 4 bp, fappofing d to be =% 6? + 3 p. 
By this means, there are two Negative 
Roots afforded, and one Affirmative ; but 
otherwife, if ¢ 7 be greater than Wd? — 5 
6? — & bp, the Equation is explicable by one 
only (Affirmative) Root. 

Fourthly, Let the Equation 27 — bz — pz 
‘\+q=0, be propofed, which has two. Affir- 
inative Roots, and one Negative, if the Cen- 
ter of the Circle be found in the indefis 
nite Space between the right Lines Pa, PD; 
- and the Curve of the Paraboloid ak that 
is, Cputting d= 5 bb Fp) aq ve lee 
than 4/d* + 35 b? -\- bp; but if 7 9 be’ great= 
er than this quantity, there is but one (Nes 
gative) Root. ee i 

But the four remaining Equations in which 
we have 1b; do not differ from thofe that 
have been mention’d: already, as to the Limi- 
tation of the Number of the Roots, if the Sign 
of the laft Term be changed, keeping the 
Sign of the third Term. But then them that 
were the Affirmative Roots-in the former, — 
will be the Negative ones here, and comtra- ~ 
riwile. Wa) 

Thus in the Equation <? —-bz* -pzmq - 
xt e, the Affirmative Roots. were either one 
or three; but in this Equation 2? be? pz 


ASE alti dae apn’ a 


“By 


— Mifeellanea Curiofa. 111 
‘\- q = 0, there is either one or three Nega- 
tive Roots, under the very fame Conditions; 
but no Affirmative Root at all. So alfo in 
the Equation 2) -\-bz?-\pz—qs0, there; 
are two Negatives and one Affirmative, if p- 


be lefs than 3 6b, and 3 lefs than /43 +3 
~ b? — & bps even as in the Equation 2? — bz? 


th pz qo, there were two Affirmatives 


and one Negative: But the quantities p and 


q exceeding thofe prefcrib’d Meafures, there 
is here only one Affirmative Root, which there 
was a Negative one. In like manner, is the 
Equation 2? bz? -pz-+-q=o0, there are 


either two Afirrmatives and one Negative, or 


one Negative only | 
Laftly, For the fame reafons in the Equa- 


_tion 2° bz? 4—pz—q=o0, there are two 


Negatives and one Affirmative, or one Af- 


firmative only, for which, in the Equation 
Re mt bx? — pz lg = 0, there were two 
Affirmatives and one Negative, or one Ne- 
gative alone; vz. aS 34 is either greater 


or lefs than /d* -\- ,> b> -\-@ bp. 


If the third Term (or pz) be wanting, the 
Center AK always falls in the Line IPEa, 


wherefore if it be <3? — bz”. y. 4 9 or 2? 4 


ba. x. tg, there can. be byt one Root, 
Affirmative if it be - 6, Negative, if -\ 2. 
But if it be 2? bz". y. + ¢ or-z3 + bz?. 
x. 9g, there may be two Aifirmatives and 
one Negative in the former, or one Affiir- - 
mative and two Negatives in the latter, the 


Center falling in the Line Pa between P and 


A, that is it.4.q be lefts, than 2707.5 for if 
it he greater, there can be but one Negative . 
in the former, or one Affirmative in the lat- 
ie an i Hitherto 


132 MzfceNanew Curiofa. 

_ Hitherto we have obtain’d the Number of 
the Roots in €ubick Equations, it remains 
that we add fomewhat concerning the quan< 

tity of the Roots. And here it is firft of all 

to be noted, that every Equation having three 

Roots, may be expeditioufly enough refolv’d 

by the help of the Table of Sines, that is by- 
_ the Trifection of an Angle, by- putting 


a/ 4b? — +p or Vad = the Radius of the Cir- | 


cle, if it be -- p in’ the Equation; or 


V£b7 +4, if — p; and the Angle to he 


Trifeéted, that which has its Sine (in the ~ 
Table of Sines) 2,0? ¢ bp tag. This — 


Angle being found, the Sine of its third. 
part, as alfo the Sine of the third part of 
its Complement to a Semi-circle; and their 
Sum, will be given from the Table of Sines. 
Now thefe Sines are to be multiplied into 


the Radius V 4 67-4 p, and thus will be ob- 
tain’d the quantities (yv& y& y& in the iz.) the 
Sum or Difference of which and + 6, as the 

cafe requifes, will give the true Roots of 
the Equation. All thefe things are deduced © 


from Cartes’s Difcoveries. But that I may — 


comprehend all the Cafes, with 4s much Bre- © 
vity as is poffible ; I fay, that the Center R, 
in the firft Formula of Equations, falling in 
the Space UGP, the two Interfedtions Y, 7; 


fall between 4 and B, and confequently ei-  ~ 


ther of the leffer Roots is lefs than 7 03 
but the third and greater always exceeds 3 b; 


but is excecded by %, But if the Centét | 


| 


Aa .7 - 7 
— Mifcellanea Curtofa. 112 
falls in the fpace G NU, there are two 
ane ' tg i i 
greater than 4 6, but lefS than ; 4, but the 
third is 8. the two others, and confequent~ : 
ly lefs than 3; but uling the Limitation o4 
the Quantity p, the Roots are included in 
narrower Bounds. For the greateft Root 1s 


eee 


‘defS than Vv Pen a pk 3 b, but greater 


than Vie b2—p-\-353 but when 3 0d is lefs 


rials / i} i hr ee / 
than p, that Limit becomes \V § 62-3 p13 4. 


oes 


‘The mean Root is always lefs than / AUT. 


“+4, but greater than }b6—‘V 42-4 ; 
but the leaft Root never excéeds this Limit, 
but vanifhes with the Quantity ¢. 


In the fecond Formulz, according to*the 
prefcrib’d Laws, there are two Afhrmative 
and one Negative Root; and the Center fal- 
ling in the Space G PE, one of the Affirma- 
tives is greater, and the other lefs than 4 @, 
but the greater exceeds not 6; but the Ne- 


gative cannot be greater than V4 bb——  b, 
and it is the difference of 6 and the Sum of 
the Affirmative Roots. But the Center be- 
ing pofited in the Space ENGa, either of 
‘the Affirmatives is greater than 3; 6, but lefs 
than / 3 bb 36; but the Negative is ever 
Vefs than } 4. But the nearer Limits (from 
the Quantity p given) aré V/ 2 UU oe Y, 
of the preateft Afhrmative Root; than 
Which it”.is always lefs, as alfo greater 

F J than 


114. Mifcellanea Curiofa. 
“than ‘VE bb—§p-L-$b5 yet the other Af 
firmative Root (which i is diminifh’d with the 
Quantity 9) is lefs than this Limit. But. 
the “Negative Root is always lefs than - 


V3 bb -\- $p— 3b, and the Quantity q be- 
ing wanting, vanifhes. 


In the third Formula, theperd are two Ne- 
gatives and one Affirmative. In this, as in 
the fourth, the Roots are not limitted by 
the Quantity 6. But the Affirmative Root is 


Doaeaecereee 


ever lefs than V4 bb- $bb--+p-+- 3, yet grea- 


ter than “f pi pa Kb 4} bs; and the greateft 
of the Negatives is always greater than 


V3 bb-LS p—%b, but lets than V poi bb 
ae 2b. But the lefs of the Negatives: is al- 
ways. leffen’d with the leffen’d Qantity ¢. 


In the fourth Formula, the Center falling 
within the Space La P D 5 if there be two 
Affirmative and one Negative Root, the 
greateft of the Affirmative Roots cannot be 


greater than von p+4 x bb “+2 4, nor lefs than 


V3 9 be +3 tp; 4. But the lefs Negative 
leis than) wea oe 
ae $bb-+-4p—}6, and greater 


than V p-+-ibb—ib. But ’tis to be noted 
here, that ‘the Negative Roots are every 
- where mark’d with the Affirmative Sine, be- 
caufe thefe are the Affirmative Roots of thofe 
four Equations, in which is found ++, andq 

= 1s 


| Mifcellanea Curiofa. . 118 
‘5 affeGted with the contrary Sine; as I in- 
timated above. © | : 

The Demonttration of all thefe things fol- 


lows from hence, that where-ever the Cen- 
ter of the Circle R falls upon the Curve 
Lines UPX or UAL, the Circumference 
of it touches the Parabola in a Point whofe 
diffance. from the Axis is / } V H, and cuts 
it on the other fide the Axis at the diftance 
of 2./}U H; but when the Center falls on 
me tiie 17 PD, one of the Roots is =o; 
and confequently the Cubick Equation is re- 
duced to a -Quadratick one, or to 22— bz 
--l- p ==0, the Roots of which give the Limits 
when the Quantity 7 vanifhes; and by how 
‘much the lefs g becomes, by fo much the 
nearer do the Roots approach to thefe Li- 
mits. The Equation is alfo Quadratical; 
when the Center falls in the Axis; that is, 
‘when 2 9 = ¢ bp — 3; 63, in the firft Formula ; 
2 9==4, 03'— 2bp,in the fecond; in) the 
third ’tis impoflible ; but in the fourth, when 
2 9 = 27 03 --% bps in which cafe the lefs of 
the Affirmative Roots is ; 6, and the greater 


Vv 3 6b -+p-l 3, but the Negative V 3 be 
a 40. In. the firft Formula, the Roots 


are 3b; and 30+ / 30) -—p. But in the 
fecond, the Affirmatives are tb, and “/ ; bb 


—p-|- 3 6, but the Negative V/ Obs peer 
And thefe things may feem to fuffice in Cu- 
bicks ; but becaufe of the excellent uft of the 
Method, by which, by the help of the T: ey 
a ee ee Se | of 


~ 


“* 


6 Mifcellanea Cuviofa. 


of Sines, the Roots of thefe Equations are” : 


a 
i 
N 


found ; I thought convenient to add an Ex- 


ample or two, by which the Compendium of 


that PraQife may be rendred manifeft. Let : 


the Equation 23 — 3922-|- 4792 — 1881 = 9, 
be propos’; and the Roots z are fought. 


3 j eREE TG / i ig 
Here V.5.60 ~ 3). Vee Nar , whofe 

double / 37 “4 is the Radius of the Circle; 

alfo 3763-1549 —% bp=2197 9405 — 311325 


Vidz 5 9% V 9% 

24. ; 
or ——--— is the Tabular Sine of the Angle 3_ 

_ 9 V 93 | 
that is, making a Divifion by the help of 
the Logarithms, Log. 9.9251560, to which 
correfponds an Angle of 57°.19.11,. The 
third part of this is 19°. 6. 24’. and of the 
Complement, is 40°. 53. 36. The Sines 


give the Logs, 9.514983 and 9.816011 35. 


which multiplied into the Radius Veer oS 
produce Y& and Y&, Log. 0.301030 = 2, 
and Log. 0.601059 = 4, but the third Y& 
is equal to the Sum of them, or 6& And 
therefore the Roots are 13-4 =5393 13-72 
— 11, 137619; @ which feveral ones 
the foremention’d Equation is compos‘d. 
Where ’tis to. be noted that the two leffer. 
Roots, do not exceed } 6 or 13, becaufe the 
Center R in the Conftruction falls on the 
right hand of the Axis that is, ¢ Op is. lefs 

than 3y'b3 4" 2 4. : Se fis 
3 For 


Mifcellanea Curtofa. 117 
For another Example, Jet us enquire out 
the Roots of the Equation +3 — 1512 — 229~ 


ssubpees Flere, V$ bb tp = V-1013= 


/ d, and the Radius of the Circle = V 405 +. 
Alfo 27 63 -T¢ op 1391251 5722 1 2622 


V ddd ro1tV tort 


the.Tabular Sine of an Arch, whofe Log: 
9.9736426, and the Arch it felf 70°. 14°. 22” 
The thitd part ‘of ‘it, is 23°. 24’: 47°34, and 
of the Complement, is 36°. 35. 12 3, whofe 
Log. Sines are 9.999183, and 9.775275, to 


which adding the Log. \/ cost, we have the 
Log. 0.903089==8, and. Log. 1.079181==!2, 
the Sum of which is equal to 20. Hence we 
ponelude that 20 1-46 or 25, is equal to 
the Affirmative Root, and 8 and 12 —3 4, 
that is 8 and 7 equal to the Negative Roots. 
But if the Equation had been +3 + 15+2— 
22.9x—§25==0, then 8 & 7 had been the Afhr- 
mative Roots, and 25 the Negative. As for 
the other Cubicks which are explicable by 
one only Root, they are to be refolv’d by 
Cardaw’s Rules, after the fecond Term is 
taken away; neither do I fee how the bufi- 
nefs can be done with lefs Calculation. 


But if this Root be defir’d to be exprefled. 


in the Terms of the Quantities b, p, q, I 
fay that in the firft Formula it is, 4.6-\- or — 
the Sum or Difference. of the Cubick Roots 


D eeetaemeanal 


of V5 qq — 405 p2 b2-4, b3 gq bpg tS, 
B73 le ote oop (viz, b ifs, 03-2 9 be 
a — I 3 ereater 


/ 


118 oo ifcellanea Curiofa, 


greater than ~ bp, otherwife —) the Sum, 


when 4 6b is greater than p, the difference — 


‘ 
4 


‘ 


when lefs. And in the other Formula, the © 


Root is always compos’d of the fame parts, 
only the Sines -\- and — being varied, as 


they will eafily perceive that are willing to 


make the Tryals. ; 
But thefe Roots are readily enough found 

by the help of the Log. Table of verfed Sines 5 

viz. if the Coefficients are furd or broken 


Nambers, and the Roots not to be exprefled « 


in Numbers, as moft commonly it happens. 
Now this is the Rule. In the firft and fe- 


cond Forimuia, if 7 bb be lefs than py tet 3? 


—bb=d, and putting the difference be- 
tween ~ bp, and 4, 63 4-4 q (that is HR) in 
the firft Formulz, and the difference between 
%6p-\ 3g and 4, 63 Gin the fecond Formula) 
Radivs, let the Angle, whofe angent is 


av d, be found. Then, as the €o-five of this 
Angle, to the verfed Sine of the fame, fo 
the Difference made Radius, to a fourth Quan- 
tity, the Cube Root of which will be had by 
taking the 3 of its Log. Then dividing 3 p — 
5 6b by this Cube Root, let the Divifor be 
fubftra&ed from the Quotient, the Remainder 
will be the Quantity Y& at Fig.1. The Sum of 


this Remainder and 56 will. be the Root, 


fought, if the Center- falls on the Right 
Hand, of the Axis; otherwife their Difference 


will be the Root. But if 3 bb be greater 


than P, making HER Radius, let-dV.d, (or 


the. diftance of the Paraboloid from the 


Axis) be the Sine of fome. Arch: let the 


verfed 


Mifcelanea Curtofa. 119 
verfed Sine of this be multiplied into Radius 
Por % ep a, 0339, and taking 3 of the 

Log. of the Produd, its Cubick Root will be 
obtained, by which let 5 65 — 43 p be divided. 
I fay, that the Swm of the Quotient and Di- 
vifor, after the fame manner added to or 

taken from 3; 6, will give the Root fought. 
And the like for the third and fourth £0r- 
mula, unlefs that 3, 3+ ¢ op 1-74 is to be 


taken for Radius, and § bb \- 4 p into Vs bb 
% ip “Or and, for the Sine. But thefe 
Rules will be perhaps better underftood by 
Examples. 

Suppofe the Cubick Equation 23 — 1722 -F 
B42. 450 = 0, and let the Root x be 
fought. Here } bb is is greater than p, but 
q is bigger than the Cube of 30, and there- 
fore “tis explicable by one Affirmative Root 


alg. Mew ~2- 3* is d>-and *57 “/222 is 
to be taken for the Sine, to the Radius a ias 
eee 433s that is *3773 and the Arch 
agreeing thereto is 15°. 30. 49. The Log. 
verfed Sine of this 8.5362376, added to the 
Log. of the Radius 2.3095913, makes 
- 0.8457889, the 3d part of which 0.2819276, 
is the Log. of the Cube Root 1.91394, by 
which, as a Divifor, dividing *3* or 4, the 
Quotient is 7.37281. The Sum of the Quo- 
tient and Divifor encreafed by the addition 
of 4 6, is the Root fought, viz. 14.9534, &c. 
" Having thus’ difpatch’d -Cubick, Equations, 
let us proceed to Biquadratical ones. Thefe 
have always either none, or 2, or 4 true 
| ] 4. Roots, 


120 Mifcellanea Curiofa. 
Roots, the determination of which depends © 
partly on the Coejficients, partly on the Sine | 
aad Adaguitude of the abfolute Number’ | 
siven. A general Conitruéion for all thefe © 
(and that eafy I] conceive enough) I have de- © 
livered at N° 188, ,which I fuppofe the Rea- 
dear to be acquainted with, but yet the 
Figure relating to that Matter, 1 think 
proper to bring hither, (Fig. 2.) In the Con- 
ftruétion of the | Equation 24— 623 pe2— qx 
Nive eget BD==16, AB==7,. 6b, BK—; 
or = the ig pene ore 1 AB=1bb, KE 
== 4 .bb Td Po AB =e S47) bb 2p, Be 
76 Oe Op, and E.G s= Feb oe Bee oie & 
Which done, a Circle on the Center 'G. with 


the Radius VG D277, will interfect the Pa- 
rabola, either in none, or 2 or, 4 Points, 
from whence Perpendiculars let fallon DH, 
will give all the Roots .z... But that there 
may be 4, ’tis evident that the Center of the 
Circle ought-to be found fomewhere within’ 
a fpace from any Point of which, three Per- 
pendiculars may be let fall. upon the Curve 
of the Parabola; and alfo that the Radius 
is lefs than the “greatelt of thofe Perpendi- 
culars, and sreater than. the middle one. 
Buc that if the Center. be pofited without 
this fpace, fo that there can be but one 
Perpendicular let fall upon the Parabola, and 
the Radius greater than it, or if it be lefs 
than the middle one of the 3 Perpendiculars, 
but, greater than the leaft..of them; : then 
there can be but two Roots only, But there 


—7 


sa no Root at all, when the Raclius VG D2—r 
¢ i 


® 


MifceHanea Curiofa, 1291 

is lefS than the leaft of the 3, or than the 
one as often as there is but one. Now it 
remains for us to inquire of what kind this 
Space is, by what Limits ’tis diftinguithed, 

and under what Conditions the Radius of 
the Circle is lefS or greater than the fore- 
‘mention’d Perpendiculars. And firft of all, 

we muit fhew how a Perpendicular is to be 
Meteora upon .the Parabola. “Let '( Fie: '3.). 
ABC be a Parabola, AF its Axis, ‘AV o 

the Parameter, G the point from whence 
the Perpendicular is to be let fall. Let GE 
be drawn perpendicular to the Axis, and 
VE be bifected in F, and erecting the Per- 
pendicular FH on the fame fide of the Axis, 

Jet FH=iGE; I fay that a Circle de- 
fcrib’d on the Génter H, with the Radius 
HA, will interfet the Parabola in three 
points, or one, z, the right Lines GZ drawn 
to which, will be perpendicular to the Curve 
of the Parabola. But now that there may be 
3 fuch Interfections, the Center H ought to © 
be fo pofited, as that it may be within the 
fpace included by the Paraboloids (in Fig. 1.) 


that is, t that FH may be lefs than s/s, FV5, 
or FH? lefs than the Cube of } VF; and 


foGE ay yey wiil be lefs than ave: VES, 

- that is, the fquare of GE will be lefs than 
4¢V E?. Therefore thefe Limits coincide 
with two Paraboloids of the fame kind with 
thofe which were ufed in Cubical Equati- 
ae, but whofe Parameter is twice lef$, viz. 
g of the Parameter of the Parabola, that is 
a of AV. And therefore it is that very 
3 Curve 


a Say 


° ae a Ta TD RRs Be 


3 | paifedie Ciriafie 


Curve Line, by the Evolution of which the 
Parabolais defcrib’d (as Hugenius has demon- 
ftrated) and which, the Line DF (Fig, 2.) 
which 1s perpendicular to the Parabola in 
the point D, is always a Tangent to.-, But 
tHe point P (that i is, that in which the right | 
Line DF touches the Paraholoid) is the Cen- 
ter of a Circle, which (being defcrib’d with 
the Radius DP) coincides with the Parabola 
in the point D, or has the fame Curvature 
with it, as is manifett. cae 


' Having therefore defcrib’d fach Parabod 
loids UXP, VNa (Fie. 2.) on either fide 
the Axis, tis clear, that unlefs the Center » 
of the Circle be placed within thefe Limits, - 
it cannot interfect the Paraboia in more than 
two points. From whence we may deter- 
mine, under what conditions, the Coeffici- 
ents of the intermediate Terms are reftrain- 
ed, in Biquadratick Equations, that fo there 
may be four Roots. And at firft fi ght ° tis 
plain that p cannot be greater than ¢ bb, 
- €viz. in thofe Forms where "tis ‘i p) nor g 
than }, 63. But in General, 7, 6? --% pb-- 
+9, that isEG. the diftance of the Center 
trom the/Axts, ought to be lefs than EH = 


a VEF, hat is (becavfe VE=#, bb -— 
 p) than 4 bb + 3p Vi, b2-- or —p, the 
Sines “+ and — being left doubtful, that fo 
they may be varied according to the nature 
of any Equation; as was fhewn above in 
Cubicks. ‘Neither would I be offenfively te- 
dious to the Learned on the one hand, nor 
deprive Learners on the other, of the Ex- 

ercife 


Maifcellanea Curiofa. 192 
ercife and Pleafure, of fending out thefe 
things by themfelves. As for the Limita- 
tion of the leaft Term 7, it cannot be found 
with the fame eafinefs, and that becaufe, ta 
let fall a Perpendicular upon the Curve of 
a Parabola, is a folid Probleme, and which 
cannot be refolv’d without the folution of a 
Cubick Equation. Therefore firft of all let 
the fecond Term be wanting, or if there, 
let it be taken away, fo that the Equation 
may have this Form 24. *. pz2. 9x. 7. mo. 
And if it be —7,, it is always explicable. by 
- two or four Roots; but that there may be 
four, the Center of the Circle ought to be 
pofited within the foremention’d Paraboloids, 
or that it may be—p, and gg may he lefs 
than .% p3 or the Cube of ; p. Then let the 
- Roots of this Equation y3.%.% py. $9 ==9, 
be gotten, the Quantities p and g having the 
fame Sines as in the Biquadratick. And 
thefe Roots are found expeditioufly enough 
by the help of the Table of Sines. But 
having found thofe three y (which are ordi- 
nately applied, to the Axis of the Parabola 
from the points, where the Perpendiculars 
to the Curve of it do fall, viz. YZ in Fiz. 3.) 
than pyy — 3y4 of the /effer y will denote the 
greateft: Quantity of 7, if it be—~+r, than 
-which if r be lefs, the Equation will have 
four Roots, otherwife but two. But if it 
bel r, it ought to be lefs than 3y4 —pyy 
of the middle y, for if it be greater, it can 
have but two Roots; at leat) ifr be lefs 
than 3y4 — pyy of the greareft y. But if 
it be greater than this, the Equation 
is not: explicable by any true Rooe at all, 
ores" : Thefe 


124 Mifcellanea Curiofa. 
Thefe fame Limits, are (otherwife expreffed 
by the Quantity 4 fy VIZ. 3 VY —y4 in the i 
cafe, y4—% gy in the fecond, and y4 + 3 qy 
in the third. But it may be, that the ae 
Yeffer Quanties y may not be far different from 
one pihaedl whence it comes to pafs that 
both of the Perpendiculars are greater than 
' the fight | Line GA, wiz. witen 41 is greater 
than’ 4 p?, but ele than? 4 <p? s phe Ente? 
falling within the er contain’d between 
the Paraboloids of 3 Figu.t. and: 2.9 Tn thie 
cafes ifs it be: Aci, "there can be but two 
Roots, y¢ b4 gy of ‘the sible: y being grea- 
ter than otherwife none. But if 4 gy—y4 
of the /eaj? y be greater than 7 mark’d with 
the Sine —, but,r be greater than 3 gy —y4 
of the mean ¥, then there will be four Roots; 
but ¢wo only, if r be found greater than the 
former, or Jefs than the latter. But if in 
the Equation it be iy Py OF if it be —p and 
4 be greater than ,4, p?, the Equation y’. *. 

= py. 4 q- is explicable by only one Root y; 
that i is, there can be but one Perpendicular 
ouly let fall from the Center of the Circle. 
Whence it,may be certainly concluded that 
there can be but two Roots only in the 
given Equation, the Sum of which, if it be 
——r, is increas’d with the Quantity rebut 
if it be +7, the Quantity y being abe dnd: 
that Quantity r ought to be lefs than y4-3 
qy, for if it be greater, the Equation pro= 
pos’d is abfurd and impoflible. 

’Twould be both tedious and needlefS to 
‘yun over all Equations of this kind, fince "tis 
evident (from what has been already faid) 
to thofe that are attentive, which are Ne- 

gative 


- 


Ait 


f ae ¥ aa BS q 

| Mifcellanea Curiofa. 125 — 
gative and which Affirmative, and that the 
Limits of thefe Roots are deriv’d from the 
found Quantities y. But for an Example 
(which any one may imitate in the reft of 


of the Cafes) let it be propos’d to difcover 
the Limits or Conditions, under which, there 


may be four Affirmative Roots in a Biqua- 
dratical Equation. Now this will be as of- 
ten as the Center of the Circle G is polited 


in the fpace UPK (Fg. 2.) and alfo tr or 


the Radius of the Circle is lefs than GD. 
Whence ’tis plain, that the Equation here 


-concern’d is of this Form, <4 —6z3 + pz2 = 


gz -+rmos; and that p cannot be greater 
than % bb, nor % pb (in this cafe) than ,*¢ 63 
“1375 again, ’tis neceflary that 40b—3 p 


in ae bb —% p thould be greater than 1% 43 
+-39—% 5p; and from thefe Lémzrs, it will 
be manifeft that the Center is contain’d 
within the fpace UPK.~ But in order to 
the determination of the Quantity x, this 


Cubick Equation muft be firft folv’d, y3. x. 


will be obtain’d the Points upoa which falt 


the Perpendiculars from the Center to the 


- Curve of the Parabola. Now having found 


the three Values of this y; the Quantity r 
eught to be lefs than 2#, 64-1 4 bq —i% bop. 
> 3y4 — 3 b2y2-+ pyy of the middle y, but 
greater than 236 6414 bg — i, bbp 1 3y4 — 
$2 y2-+- pyy of the leaft y. But if r exceed 
thefe Limits, there can be but two Roots 


_ obtain’d. Laftly, if 2$, b4-+ 4 bp — x, bbp 


3y4 —=% bby a pyy of the greatelt Vy be grea- 
ter than 7, then the Equation propos’d 1s 
im- 


126 0 =Maifcellanea Curiofa. — | 
~impoflible’ It happens alfo that there aré 
four Affirmative Roots, when the Center G 
is pofited in the little fpace UTS, viz: 
drawing RTS perpendicular upon the mid- 
dle of the fuppofed Line AD. But this 
comes to pafs when p is greater than ,& 00, 


and % bb —}p / i bb —<% p greater than § 

pb —1i, 63 —449. In which cafe always two, . 

_fometimes three of the Roots are greater 
than 4b. | Dar ays ; 

But ’tis to be noted here that that Limit 
‘produced from the /ea/t y, is fometimes Nes 
gative, or lefs than nothing , wz. as often 
as the greateft of the three Perpendiculars is 
greater than GD (Fig. 2.) If this happens; 
the Quantity --r may be dimintfh’d to no- 
thing from the Limit prefcrib’d, by the 
middle y. But the defect of a Limit from the 
leaft y, fhews how great —r may be in the 
Equation, if there be three Affirmative Roots 
and one Negative one ; which if it exceeds, 
‘there can be but two, one Affirmatsve and 
the other Negative. And all thefe things 
are demonitrated from hence, that the fore- 
mention d Limits of the Quantity r, ave the dif- 
fevences of the Squares of the Line GD, and the 
Perpendiculars to the Curve of the Parabola. 

But becaufe of the perplexing Cautions ari- . 
fing from the diverfity of Sines with thefe E= 
quations, ’tis better always to take away the | 
fecond Term, and then to inquire out the 
number of Roots and the Sines, according to 
the Rules already deliver’d ; efpecially if thofe 
Quantities y are not much different from oné 
another. But of thefe four Affirmative Roots, 

: : : EWwo 


ore 


et gale 1 Se 


ea en a Smarr f > aeneiieendian: ofa oe 
es : ‘ r ae 4 eo’ ey 


% i ; : ” 
> mls 5 : | . ; 
é 7 ; | | | 
7 . ‘ : 
| | 3 L 
k , al i / 
i - 

i _ | 

; . | | | 
j f 7 

Z) $ : | | 
{ 7 ; ; : 
. F . i 
‘ ‘ - : j - - : ; | 
} | e 
, | | 
; | | | | 
+ 
. . 
‘ 4 
j . 
= i 
4 i ; 
> 


A= 


aos pl ime 


Maifcellanea Curiofa. © 127 
two are always lefs than 4 b, and two grea- 
ter, viz. if DG be lefs than AG, or % pb than 
é, 63-4. But three are always lefs than § 4, 
as often as the mean Perpendicular (or that 
found from the mean y) is greater than AG, 

org bby greater than 3y3-—pyy of the fame 
mean y. The fourth and greateft Root is 
greater than the greateft y 1-4; and “tis 
equal to the difference of 4 and the Sum of 
the other three Roots, and therefore is .lefs 
than 6. ve 

_ But ’tis now time to have done with this 
Matter. Perhaps thofe that more perfectly 
underftand the Nature of the Parabola, may 
be able to do all thefe things after a more 
compendious manner. But there is fome 
caufe to doubt, whether all thefe Quantities- 

6. p, 4.7. can be rightly determin’d without 

the Refolution of a Cubick Equation, or no. 
For whatfoever is done in Plain Equations in 
this Matter, exhibits, not the true Limits, 
but fome Approximations only. 


Some 


128) | Mifcellanea Curiofa, — 


‘Bove Tilaftviots Specimens + af thé 
Doctrine of Fisscmuen 3 or fixe 
amples by wibich 4s clearly 
afhewn the Ufe and Excellency 
of that Method in folving Geo- 


metrical “Problems. 


By Ab. De Moivre. 


OU have here alfo the Method tk 

I promis‘, concerning the Quadratures 
of Curvilineal Figures, the Dimenfion of 
the Solids generated by the Relation of a 
Plane (and of the Surfaces) the Redtification 
of Curve Lines, and the Calculation of the 
Center of Gravity. I know thefe Points 
have been already handled by feveral very 
learned Men—- But I hope this At- 
tempt of mine will neverthelefs net alto- 
gether difpleafe, if (efpecially) I have had 
the good Luck to find a fhorter and more | 
expeditious way to thefe things, than what 
is commonly known. 

But before I proceed farther, I would 
have it obferv’d, that I make fe here, of 
what the celebrated Mr. Newton has de- 
monftrated, Page 251, 252, 253. Princ. Phil. 
- concerning the Momentaneous Increments. or 
Decrements, of Quantities that Increafe or De- 

crease 


| Mifcellanea Curiofa: 129 


creafe by @ continual Flux; Efpecially, that 
Le 


the Momentane of any Power, as A m™ is 
gt 23 | 
n ei Ue ngs 
em, a AA 7 a. Partners “the Fluxion en 
en ae : 


-a/4L" being given, the flowing Quantity 


7 n 

A™ may be found; Firft, By ftriking a 
out of the Fluxion;, Secondly, By encreafing 
the Index of the Fluxion by Unity ; Third- 
ly, By dividing the Fluxion by the Index 
thus increafed by Unity: In the following 
Difcourfe, we fhall exprefs -4b/ciffe of any 


Curve by x, its Fluxion by x, the ordinate 


by y, and its Fluxion by y. Thefe things 
fuppos’d ; that we may come to the Quadra- 
ture of Curves, Firft, Take the value of the 
ordinate applicate, by the help of the Equa-. 
tion exprefling the Nature of the Curve: 
Secondly, Let this Value be multiplied by 
the Fluxion of the Abfcifle; for the Pro- 
‘du& arifing is the Fluxion of the rea. 
Thirdly, Having the Fluxion of the Area, 
Tet the flowing Quantity be found, and fo 
we fhall have the Area fought. Ex. gr. Let 
mn 

the Equation x ==y be propos’d, which ex- 
prefles the Nature of all forts of Paraboloids. 
< 4 mn 

The Value of » is «” which multiplied by 
: K nia 


120 Mife ellanea cuetiha. 


‘x, gives a? x st the Fliciog of the Aree 


“ 
and confeanentiy the Area fanght is —— 


m+n 
jt | =) 
x , or Cfubftituting y inftead of W 


X Ye 
m-|- iL 

Again, fuppofe a Curve, whofe Equation 
is x? + aaxx yy (which is the firft of the 
Excellent Mr. Craig’s Examples) putting a 


e Met My ‘aa, the Eluxion of the Area will be 


eee ee 


we ob ‘aa. Which Expreffion involving 
a furd Quantity, let us ice “xe aaTa, 
then will xv" aamx*, and confequently 
xe mzzZ3 and fabititetioe zx, and z for xx 


—st 


and oy + an, the Fluxion thus freed from 
Surds, will be x” 2: ; which reduced to its Ori- 


ginal; 2? and putting V xa-t-aa for z, we have 


“2 ya\aa V xx aa for the Area fought. 

~ But to fhew more effectually how eafily 

thefe Quadratures are perform’d, I fhall add 

one Example | more. Let the Equation of the 
ag? 


v 
Curve be : = y*, therefore y = ——, 
‘ ae 7 ; one 
: : me Varka 


et ae : Fae eae Rca ‘ ‘ P e i biog 
and therefore ———-_ is’ the’. Fluxion of the 


“/ x'\"Aa | Area. 


: Mifeellance c ur 0 


Area. Put: Moet fam a hence KHL a 


Pe by 


we 


F272 et 2AZe 


alte! #t2zz. Therefore 
poe 


and confequently 3; z>-—242, or ; cf a4 
Vela will be the Area fought. 


But it often happens that we meet a 
fome Curves (fuch as the Circle and Hyper~ 
bola) which are of fuch a Nature, that ’tis - 
in vain to attempt the freeing the Fluxions 
of them from Swrds. And then reducing 
the Value of the ordinate into an inf- 
mite Series, and multiplying the feveral 
Terms of the Series into the Fluxion of 
the Abfciffe (as before) let the Hiuent of 
each of thoie Terms be found, and fo there 
will arife a new Series, which will exhibit 
the Quadrature of the Curve. 

This Method is with the fame cafe appli- 
ed to the Menfuration of the Solids generated 
by the Rotation 0° a Plane; viz. taking for 
their Fluxions, the Produ& of the Floxion 
of the Abfcifle into the circular Bafis. Let 
the Proportion of a Square to the infcrib’d 


Circle be —..- The. Equation. exprefling the 
I ; | | 
Nature of a Circle is yy = dx 44x; there- 


fore 4 dxx -~ x? x is the Fluxion of a Portion 
“ : Ki 2 of 


4 
\ 


132 : _Mifcellanea Curtofa. 


of the Sphere, and confequently the Portion 


Yee ees an 
= * 
rie 


it felf is 43 dx? 4 4x3, and the circumfcrib’d 


‘ “a 
Cylinder is 4 dx? — x3. Therefore the Por- 


17 ; 
tion of the Sphere is to the circum{fcrib’d Cy- 
linder, is ast d—3xtodex. 

The Reétification of Curve Lines will be ob- 
tain’d, if we confider the Fluxion of the 
Curve as a Hypothenufe of a Rectangular 
Triangle, whofe fides are the Fluxions of 
the Ordinate and Abfciffe. But in the Ex- 
preffion of this Hypothenufe, care muft be 
taken that only one of the Fluxions be re- 


- maining, as alfo only one of the indetermi- 


nate Quantities, viz. that whofe Fluxion is 
retaind. Some Examples will render this 
clear. : ons 
(Fig. 1.) The right Sine CB being given, 
to find the Arch AC. Let AB=x. CB=y. 
OA=r. CE the Fluxion of the Abfciffe, 
ED the Fluxion of the Ordinate, CD the 
Fluxion of the Arch CA. From the Pro-. 
perty of the Circle 2rx—x«x = yy, whence 


ari me 24x 2yy, and therefore xi yy. But 


at ae a 
CDizytaxaytyy mayb 

| i rm are ex. 
o ret | ita 
yyy rryy 5 :‘therefore CD = --—-——- 
Ue eestaipsonn ted yg Lb Sa 
17 em Vy iT yy Vir py 
= 


mom 


ee eS 


Maifcellanea Curiofa. 133 
I 4 : y i : i 
See yy x my. «And 
Vir=yy | 
confeqnently if rr —yy be thrown into an ine © 
“finite Series, and the feveral Members of it 


be multiplied into ry, and then the flowing 
Quantity of each be taken, we fhall have the 
length of the Arch AC. After the fame 
manner, giving the verfed Sine, the fame 
Arch may be found. For refuming the E- 


quation found above 2rx— 2x = 2yy, we 
have y Fire wx, but CDisxx hy swe 
Ys 


TKK we WX RN NM 


— ee 
Uae ae 
rrxn ms 2rexe Te? eK 
—g—-———- ————, that is, (reducing all 
2re x8 | 
to the fame Denominator, and expunging 


ha TVX 
contradifory Terms) ————~, whence 
es 2K mm HH - 
CD= re ~— ; and confequently the 


PR) RTT ETD ony 


“hia M orm xx . 
length of the Arch AC may be eafily found 

from what is faid already. : 
Aut ' K 3 : The 


(134 Mifcellanea Curwfa. 

The Fluxion of the Curve Line is fome- 
times more .eafily found by comparing the 
two fimilar Triangles CED, CBO, for this 
Proportion arifes, CB: CO: : CD; that is 


et 


for the Circle NE bye axe: Tt 1K 


Af UK ARK. 
The Curve of the Cycloid may be deter- 

min’d by the fame Method too. Let (Fig. 2.) 
ALK be a Semicycloid, whofe generating 
Circle is ADL. Having any point as B in 
the Diameter AL, draw BI parallel to the 
Bafe LK meeting the Peripheus of the Cir- 
cle in the point D, compleat the Rectangle 
AEIB, and draw FH parallel to EI and infi- 
nitely near to it, as alfo BI cutting FH in 
G, and the Curve A in -H. Pot AL ed. 


AB(= El) =x. GH= x. It is known that 
the right Line BG is everywhere equal to. 
the Sum of the Arch AD and the right Sine 
BD; whence ’tis manifeft, that the Fluxion 
IG is alfo the Aggregate of the Fluxions of 
the Arch AD and the right Sine BD. “But — 
the Fluxion of the Arch AD, was found 


sdx and the Fluxion of the right 


———— 


Leal ne eae 


a ep co wae 
Sine BD will be found to be. dic m 2a 


| Oe ge el 
therefore - IG = Mee hm 0 and therefore 


aes 


Ndi Hy | ee 


— Mifcellanea Curwfa. 035 


| TE] ( sia Gil) = despots Meals ; from 


dm xx 


Baad ait oT. foe 


de eX x 


pl» 


4 


and confequently Al m2d« =2v/d«x=2AD. 
This Conclufion may alfo very eafily be .de- 
daed from the known Property of the Tan- 
sent... For fince the little part of it, as 1H, 
‘5 always parallel,to the Chord. AD, the 
Tclangles IGH, ABD are fimilar, ~whence 


AB: AD:: GH: IH, that isa Vda ck: 


ergy) 3 wort (a1! ane 
xJde, therefore IH maV/dx dx x. By 
oe ae 


the help of the Fluxion IH alfo, we may 
inveftigate the Area of the Cycloid. The 
Fluxion of the Area AKI, is the Rectangle 


HIG dex — xx. xVde a xx. But the 


Fluxion of the Portion ABD is the fame; 
therefore the Area AEI and the correfponr 
dent Portion (of the Circle) ABD, are: ae 
ways equal. RELUISe iW BGA 

a , a cu 


W's 


1360 Mifcellanea Curiofa, = 
Let AB (Fig. 3.) be the Curve of the Pa-— 
rabola, whofe Axis is AF, Parameter a; let 
AE= x, EB=y, AB=x, BD=x, DCxy, 
BC=x. The Equation exprefling the Na- 
ture of the Parabola, being ax =yy, we have 
ee Wy whence x ayy 5 but BC? = BD4 
i a 


eo 
2 


1 tph, thie i'd eae eee 


aAa- 


ayy Te aayy, and therefore Pe 7 V ay? + ad 


. - : 


Aaa 7 Bs 


=y Vy --iaa. If now by this Expref- 


z 
2 4 


fon y Vy + 4 4a be thrown into an infinite 


Series, the Curve AB will eafily be known. 
It appears farther, that giving an Alyperboli- 
cal Space, this Curve is alfo given, and wice 


-werfa. For } az cy Vy -- 4 aa, and confe- 
quently 3 4x is the Space whofe Fluxion is 


el y* -\'G aa.” But fach.a Space is no other 
than the Exteriour ' (Equilateral) Hyperbola 
ABEG, whofe Semiaxis AB =4 4, its Ab- 
- fcille AE =y, and its Ordinate EGmx. 


For 


Mifcellanea Curwfa, 137 

For the Menfuration of @ furface defcrib’d 
by the Converfion of a Curve round its Axis> 
we are to affume for the Fluxion of it, a Cy- 
lindrick Superficies, whofe Altitude is the 
Fluxion of the Curve, and whofe diftance 
from the Axis is the Ordinate Applicate cor- 
refponding to that Fluxion. Ex. gr. Let AC 
- be the Arch of a Circle, which turning round 
the Axis AD, generates a fpherical'Superficies, 
which we would meafure. Now DC the 
_ Fluxion of the Arch is already found to be 


rx 
= ————, which if we multiply by the 
pune ; 


Periphery belonging to the Radius BC, that 


is, by £N are xx (putting + the Ratio of 
the Circumference to the Radius) we thall 
have cx for the Fluxion of the fpherical Su- 
perficies, and confequently that Superficies it 
io, is tx. . rae 


As for Centers of Gravity; having gotten 
the. Fluxion of the Solid or Surface, and 


_ multiplied the fame into its diftance from 


the Vertex, the flowing Quantity muft be 
found, which divided by the Solid or Surface. 
it felf, the Quotient will fhew the diftance of 
the Center of Gravity from the Vertex. Thus 
to find the Center of Gravity of all the Pa- 
_faboloids; their Fluxion is thus generally 

Fa | 3 expreiled 


178 a Criofas | 
4 im 

etpriee ® “ which multiplied by x, , makes 
a te 


Be i the doings Quantity of which, 


* ae ao | 
ViX, —a—— KE divided. by Set Area P56 
mr-\- 22. i Ch A y 
m~\~ 1 
Ayla m-\-2n- 
the Paraboloid 2) bi BO = x, 
- men man 


the diftance of the Center of Gravity from 
the Vertex. 


The Center of Gravity of a Portion of a 
Sphere, is found after the fame manaer. } 


al 


its Fluxion 4 dxx—.x’x multiplied into «, 


4 


makes 4 dx?x— xx, whofe flowing Quan-. 


ap 


‘tity 4pae! — 2 ae? Bp he eee 


2 


Content of the Portion, vz. 4.3.dxx—3 x's 


wa : 


pa 4% 4d — 3% 
gives 


3 K—c, OF 
2a—3% 6d — 4x 

flance of the Center of Pp erie from the 

Vertex. 4 : ; ine teh 


xy the ‘di- 


—— Mifcellanea Curiofa. 139 
‘My defign here was not to be large, and 
purfue all the Difficulties that may oc- 
cur. 7Lis fufficient to have made a be- 
ginning, and led the Way to thofe greater 
Pranss..s> a 


Hee oti 4 MMe-— 


149 Mifeellanea Ciriofan 


4 "Method dof woe ane fois 
of Curves, or Reducng them 
to more fi mole Curves. 


by A. De Moivre, R.S.S. 


ET A be the Area of a Cane whofe 
- Abferffe “1s ¥, and Ordinate” Applicate 


x ae —xx. Let B be the Area of a Curve, 
whofe Abfciffe is the fame with the former, 
m= 


and its Ordinate x Mdee — xX. Put 


Viswas “x =e a4 basse ae “eS aa ad B into 
am-|-r. 


am-|-4 


ah Socae 


ae 


AON d to 2m-\-1 soe 3 | 
- ahi case y =e 


z 


a at gg 211—I a 
— in 10 “ts jin awe a =— 5 
—“ 2m-|-1 m—t . ome 


got into 2m-\-4, into 5 2m-|-2 218 


x ys es eu, dec. 


Where we are to Note, 1. That z is fup- 
posd to be an ‘Integer and Affirmative 
bi oe a. That the Quantity d”B,.in the 

| Series 


™ 


Maifcellanea Curiofa. 42 
Series exprefled by P, is to be multiplied in- 
to as many Terms as there are Unities in z. 
3. That as many of the following Series ex- 
prefled by -Q.,—-R,—5,—T, &c. are-to be 
taken, as there are Unities in. Which_to il- 
‘Iuftrate by an Example ortwo: If#=i, the 

eth ol See Oo gk 

I fay that Ard”B. deben Sela “Tie | 3g 
x rt: 


and if #=2, then A=a”B into 77) into 


2n—2 Ms I tml» a _d. A 2m-t 
ee ae oe 
“23, 4. That if y be put SV de + xx, 
then A will =Q~—-R-+S-—T, &e. AP. 


CO ROL. i: 
If m be put = to any Term of the follow- 
ing Series %, 2,25 2> 2) 2» &c. then the 
Quadrature of the Curve whofe Ordinate is 


x ae xx, OY X Vf dic -|- «x, will be ex- 
prefled in finite Terms, and be found by 
our Series. To illuftrate which by an Ex- 
ample or two; Let it be required to 
find the Area of a Curve whofe Ordinate is 


4 V dee — xx. Let us imagine this Curve 
to be compar’d with another Curve whofe 


< 3 eigen a 
= C @ ae e 
Ordinate is x os —xx. Now becaufe in 
this cafe 2 =i1, therefore will Am d’B into 
Qm-i Ll Mem td | i : 
geeks mie” 73 But mma ENS 
| fore 


142 Mafcellanea Curiofa. | 


fore 2m-—-1=0, and thesefove A pa 
De = =i ays 


av x3. 


It is here to be obferv’d, that the Area — 


thus found, is fometimes deficient from the 
true Area, by a given Quantity, or exceeds 
it by that fame given Quantity. And in or- 
der to find that. Defec& or Excefs, let the 
Area found be fuppos’d to be encreas’d or 
diminifh'd, by a given Quantity g, and then 
putting + = 0, let the ie increas’d or di- 
minifh’d, be fuppos’d = Thus i in the pre- 
fent cale, we fhall find 7 3.4V/d, and con- 
fequently AS 3 afd — 2y> 


ans 


COROL. I. 


If z be put equal to any Term of the 


following Series; 3574,, 5) 6, 7 Ce tem eee 
Quadrature of of the Curve whofe Ordinate is — 


7 
x Vide — xx, — xx, Or x ii alist =X, 1S expref= 
fed in finite Terms, and is eis. ’by our Se- 
ries. 


Let the Area of the Curve he to be 


found, whofe Gidina td is “x ego oa Ce 


Suppofe it to be compared with the Area of 
‘a Circle, which call 4. Then will m =o, 


2 3, and foo AM P-Qo#R-S. But | 


fince, in the Denominator of the third Term 
‘ by which 4B is multiplied, there is found 


mr ick 


Mifceanea Curiofa. 142 
2m, a Quantity infinitely fmall, or rather . 
nothing ; the Quantity exprefsd by P is In- 
finite; and for the fame reafon the Quan- 
tity exprefsd by —S is Infinite, and {6 the 
_ Quantities A, ~Q, —R, do vanifh. There- 
‘ fore P=S, and dividing the Equation by 


2m-\-1 2m—t1 ° ane 
into ———) we have d”B into d 
2m-\-4. 2m-|-2 | : ied 
dd’ m—3 20-3 Us at. 
ic rt 4 3 : 7 ——— > * 3 e 
mow. “y?, or 4B into —~ mddx 


and putting o and 3 for and #, there will 
be dB into -2=y3?, or B= — 2y?. 
“P gx03 


COROL. III. 


If m be put equal to any Term of the fol- 
lowing Series, —2, 1, 0, 1, 2) 3945 5, &c. 
the Quadrature of the Curve, whofe Ordi- 


nate is « V ade —xx, depends upon the Qua- 
drature of the Circle. But the Area of the 


im” Papen pam ene 
Curve, whofe Ordinate is + V dx-Lxx, de- 
pends upon the Quadrature of the Hyper- 
bola; and the relation of that Curve to the 
Circle of the Hyperbola, is exhibited by our 
Series in finite Terms. | 


‘COROL. 


Mw:e 


TTS ER nS aa ate eR 


144 Maifcellanea Curiofa, 


COROL 


mail. 
’ 


“If m be expounded by any other Term; | 


different from them already mention’d; the 


Curve whofe Ordinate is *, Viasat: or 


cc ene : i rig Ar 
x NL die + xx, 18 Neither exadtly fquar’d, nor 


does it depend upon the Circle or Hyper- 
bola, but is. reduced to a more fimple Curve 
by our Series. | 


: THEOR. If 


Let A be the Area ofa Curve whofe Ab: 


re 


fciffe is x, and Ordinate Vde — ax. Let B 
be the Area of a Curve whofe Abfcifle is 
the fame with the former, but the Ordinate 
m—n ; ; 
x : 


NI dex mixx Let Vda xe =, | Then will 


Mifeellanea Curiofue 145 


: a ae. M3 C= 2m—5 . 
A=d"B into into into cn) into 
| 2m 2m——2 -2m—s. 
2m—7 = 
2m—6 SS 
“2 m—r 
—_-— NX ee vet 
in 7 
| ae 2M—1 Mee 
——— Into Ls <= R. 
m— 
dd a 2° mt 
a ee nto y= 
RO 4 | Loe ae 2M~——3 . 2m—s5 
— .— Into ——— into into 
m—3 2m 2m—2 2m—4. 


m 


Pe of “y=eT, XC. 


| The Obfervations to the firft 7 heoren, take 
‘place here alfo, as in what follows. 


GOROL 


if m be put equal to any Term of the 
following Series, 3,3, 2) 3.2, &c. the Qua- 
drature of the Curve whofe Ordinate is 


- mM ‘ m 
ive x 
———, or ————-, is exprefled in 
! MV de — 0 V dex —|- 2" 


finite Terms, and exhibited by this Series. 


7 


boo in oo COLO L, 


146 - Mifcellanea Curiofa. 
COROL. I. 


If x be put equal to any Term of the fol- 
lowing Series, 1,2, 3,4, §, 6,7, &c. Every 


; x 
' Curve whofe Ordinate is ———, OF 
af dum 
—— 
ie ® ® e 6 
—————, is fquared by this Series in finite 
MV docs 
Terms. 


GORE ee 


If m be expounded by any Term of the 
following Series, ©, 1, 2, 3) 4) 5) 5) 7, &C. 
m 
: : x 
the Curve whofe Ordinate is —————-, de- 
AN mK 
pends upon the Quadrature of the Circle. 


m 
xe 


But the Curve whofe Ordinate is ant iy 
| Video 4 sie 
depends upon the Quadrature of the Hy- 
_ perbola. 
For if on the Center C, (Fig.20.) the Diame- 
ter AB=d, the Circle AEB be defcribed, and 
AD be taken =~, alfo erecting the Perpendi- 


* cular DE, the Line CE be drawn. Then the 
: Se3 


| — MifceHanea Curiofa. 147 

Sector AEC divided by 34d is equal to the 

Area of the Curve whofe Ordinate is 
saa “ 

——emn—m——-, After the fame manner, if on 


Wiad tiie’ 

the Center C, and the Tranfverfe Axis 
AB=d, the Equilateral Hyperbola AE be 
defcribed, and taking AD-==., and eredting © 
DE at right Angles, and joining CE, the 
Sector ACE divided by {4d is equal to the 
Area of the -Curve whofe Ordinate is © 

0 j F 


(oe ea © Rea = 
i ¥ A ~ 


COROL. IV. 


If m be equal to any Term, that does not 
fall into the foregoing Limitations, then the 
| wn : 
Curve whofe’ Ordinate is ————,_is_nei- 
) ; : V dic-beexe , . 
ther exactly fquar’d, nor does it depend up- 
on the Circle or Hyperbola, but is reduced 
to a more fimple Curve. 


1; Z THEO: 


148 - Mifcellanea Curiofa. 
THEOR. TL 


Let A be the Area of a Curve whofe. 
Abfcifle is x, and its Ordinate Applicate — 


ve a ‘ 

x MV rr—xx 5 let B be the Area of a Curve 
whofe Abfciffe is alfo x, and its Ordinate 
2d | | 
x VT —'XX » 


occ 


aoe! 


Let Vir—xx—y. Then will A=/"?B in- 


ce 5s 26h 
to | i into into’ inte 1 xe a 
Mt | 
re Oy ae 
m\-2 Ha — ems C7. : 
Tx: w—t M—32 7 
ee a into 2 x —R 
74 ti—-2 —3 m— 
a into —— into x y3 =—5 
: 2 2 a eakts = 
&c. peer 
ae he 1 
G.0 B.C. 


If m be expounded by any Term of the 
following Series,-1,3, §; 7, 9, &e. the Qua- 
drature: of the Curve whofe Ordinate is 


ij ————— YL pment 

at ae or x Nils la is had in finite 
Terms, and that by the help of this Theo- 

rem. a 


e q 
we tea ke he 


COROL 


| Mifcellanea Curtofa. 149 


£0 ROL vit 


If m be expounded by ae Term of the 
following meries, 2-49, 4, 5,6, &c. then the 
oy 


—~ 


_ Curve whofe Ordinate ts x Nye be or 


io 
ele aex: Coes is exactly {quar'd by this 
' ‘Toren. 


COROL. IF. 


If m be expounded by any Term of the 
following Series, — 2, 0, 2,4, 6, 8,&c. then 
_ the Quadrature of the Curve whafe Ordinate 


piscx lk ee, depends upon the Circle, but 
the Quadrature of the Curve whole Ordinate 


iS x TA si dea |-aeee, ee upon the Hyper- 
bola. 


COROL.: IV. 


If m be expounded by any Term differ- 
ent from thofe already taken notice of; 


at 


then the Curve whofe Ordinate is + Weg 


| m nn: 

or x Vert wx, depends neither upon the 
_ Circle nor the "Hyperbola, but is reduced to 
amore fimple Curve. 


O35) 3 THEO- 


150 © ~ Mazfcellanea Curiofa. 


THEOR. IV.) 


Let A be the Area of a Curve whofe Ab- 
: i . 7/3 : 
: : iis 
fciffe is ~, and whofe Ordinate is Rae 


Se 


let B Lote the Area of a Curve whofe Abfcifie 


M—27 


x 
is alfo x, and its Ordinate —-——. Then — 
| Vee 


° e N—=f e m— e ; / Naw 
will A=r2"B into —— into "= into et 
m m—A m—Z4 


6 
rt m—!I 
poe a y= 2. 
¥ M—1 3 
— into —— « yu—R. 


r4 Nn . 
———— into — —— : into’ x aa! 
m4. m m—2 ae ils 


76 


® M—— tT ry } wi--- ° Y 4 aaa estates tbat 

me ——— Into —— into.—— into ssi a ’y 

bs ie Mio Mis ag els ied m—4. | 
=— T. ke. 


COROL. 


—  Mifcellanea Curtofa. 151 


PeCOROL 1. 


If m be expounded by any Term of the 
following Series, 1,3, 5, 7, 9, &c- the Qua- 
drature of the Curve, whofe Ordinate is _ 


: m 
a, 


——, is obtained in finite Terms by this 


i a 
Theorem. 


£0201. i. 


_ If » be expounded by. any Term of the 
following Series,.1, 2, 3) 4) §, 6, &c. the 


—= 27 
Fe, 


or 


Curve, whofe Ordinate is 


Cae 


is {quar’d exadly by this Theo- 


—2n 
Pe aa : 

P) 
| Vereen | 


COROL. IIL 


If m be expounded by any Term of the 
following Series, 0, 2, 4, 5) 8 10, &c. the 
“Quadrature of the Curve, whofe Ordinate 
meds : L 4 : 1s 


is2 = Mifcellanea Curiofa. 
\ ae uff . ; : 
is ——--_ depends upon the Quadrature 
eS | | ed 
of the Circle. For if on the Center C, and 
the Radius CA=r, the Circle AEG be de- 
ferib’d, and taking CD==*,. DE be erected 
perpendicular to CD, :and.CE be drawn ; 
then the Sector CAE, divided by v5 7%. (187 
equal to the Area of the Curve, whofe Or- | 
O- 


n | ‘a 
dinate is ip tee manner, (Fig.21-) | 


id ae | 


if on the Center C, and the Scnieventvertey 
Axis CA=r, the Equilateral Hyperbola KAM 
be defcrib’d, then drawing CF -perpendicu- 
lar to CA, equal to x, FE parallel to the ~ 
Axis till it meets the Hyperbola in BE, and 
join CE; then the Hyperbolical Sector ACE 
divided by : eis equa! to he Area of the 


x 


he HR 


COROL. “I. 


Curve, whofe Ordinate is 


If m be expounded ie any Term diffe- 
rent from the OTEE ONDER then te Curve, | 


x: d 
whofe Ordinate is -_—__., is inpaehier ex- 


Virx-ex ie 


adly 


| ~Maifcellanea Curiofa. 153 
aGly fquar’d, nor does it depend upon the - 
Circle or the Hpperbola, but is reduced to 


a more fimple Curve. 


THEOR.. V. 
Let A be the Area of a Curve, whofe Ab- 


: {ciffe is x, and its Ordinate —— ; let B be 


ee . 
the Area of a Curve, whofe Abfciffe alfo is 


ye s 
_x, and its Ordinate —-—. Then will A= 
f Lomas NO aa 
eee ee dx" dn , 
d*B— fey ee ee et ee ccc, 
m M—1 m—2 
/ ; ax 
Let the Ordinate be ——., and then the 
| Fel d-\-x 


eae ddan 3 
Area A will = —~——--— Hj eee eC. 
; ™ i— 1 M—— 2 

a”B. 


2 OR OL: 


If m be expounded by any Term of the 
following Series, 1, 2, 3, 4, §, 6, &c. the 
Quadrature of the Curve, whofe Ordinate | 
Bia cM i, 
is —— or ——, depends upon the Quadra- 

dum X mI 
LO ew. ture 


» 
wassa eer 


454 Mifcellanen Cariatth 


ture of the Hyperbola. For (See Fiz. 22.) | . 


drawing DE, EF at right Angles, take EG 
=—<d, and draw GH at right Angles to EF, 
and equal to it. Wa£thin the Afymptotes 
DE, EF, let an Hyperbola be defcrib’d, 
pafling through the point H; which done, 
take GK—=~, towards EF in the firft Cafe, and 
towards F in the fecond; and draw the Or- 
dinate KL. Then the Area HGKL divided 


by dd, is equal to the Area of the Curve, © 


x? x? a 

or ——. Hence the. 
, dex d-|-e¢ 4 oay 

Solid generated by a Portion of the Ciffod, 

while it turns about the Diameter of the 

Generating Circle, is exhibited in finite © 

Terms, fuppofing the Quadrature of the Hy- 


perbola. 


whofe Ordinate is 


THEOR. VL 


Let A be the Area of a Curve, whofe Ab- — 


el 
icifle is x, and Ordinate — : tee Be be: 
|x 

the Area of a Curve, whofe Abfcifle is alfo 
gel —an 

x, and Ordinate Then will the 

rr—\-x% Seobh 

an rex 3 ty) | 

Area Boe me ee ee fee KC, 
Mormon Mm 3 M—5 | 


he r2"B. 


COROL. 


s + 


Mifcellanea Curiofa. 155 


COR OL: 


If m be expounded by any Term of the 
following Series, 0, 2, 4,6, 8, &c. the Qua- 
drature of the Curve, whofe Ordinate is 
oP og : . 
——-, depends upon the Reétification of 
yr-|-4N 
the Arch of a Circle. For defcribing the 
Circle AEG on the Center C, with the Ra- 
dius CA= 7, draw the Tangent AK—~, and 
join CK meeting the Periphery in E; then 
the Arch AE divided by 7r is equal to the 

x 

Area of the Curve, whofe Ordinate is - 

is : rr—|-oce 


General Corollaries to thefe fix Theorems. 


Very Mechanick Curve (whofe Quadra- 
ture depends upon any one of that In- 
finite Number of Curves, whofe Ordinates 


Gremearcest: teem? 


have the following Forms, « M dic bax , 


x x 
REET eg Cee : Yl see - UL Pa) ; 
ies es 9 
i VITNK sy, 8 ae dx 
Vide xx | 
xt 


-) may ‘be fquar’d by thefe Series. It 

rr-|-xeF : 

may fuffice to illuftrate this by an Exam- 
ple. : | 7 


_ Sup-* 


156 Mife eVanea Curiofa’ 


Suppofing the Cube of the Atch of a Cir- 
cle (correfponding to the verfed Sine) to be 
the Ordinate of a Curve, whofe Abfciffe is | 
the fame verfed Sine; let it be peguir to 
find the Area of this Curve. 

Let the Abfcifle be «x, the Gikentar Arch 


ers then the Fluxion of the Area is cad fet 
the Area be v?x—J. ‘Therefore v3 x2-|-30? 


Ug e, whence g == 30? UX. Baik hc 


re oo ie SO Auar ae 

nae , therefore 7 = - —-. But 
a ees ges Byer re 

: Re ue dx 
(by Theor. 25) : a i — 


Wie pues Vives 
yar); ; and confequently 4 = ddv?u—3 


dv* Vs therefore 74V3—5: doy. There- 
fore now we are come to es that the. 


Fluent, of the Expreffion 34v” Yo is to be 
found. 3 | 
Let this Fluent be jdv*y—-+. 


Therefore idv’y-[-3dvyy—r—hdo?y. | 


And confequently r= aduvy=tddex. & 
Let y= ddvxr—s. 


Therefore stdpe-t dae caauee 
ae And 


Maifcellanea Curiofa. 157 


303 xx 


Romer © Geel 


ee 1) 
mS Seales} (by Theor. 2.) Therefore now 
s=jd?u—jd3y. And confequently the Area 
fought, es x td! | jdv7y—jddvx-|-,d3 
’ v—id>y. 


And pcanena s—tddev= . 


Since the Solids and Surfaces generated by 
the Rotations of Curve Lines, as alfo the 
Lengths of Curves, and the Centers of Gra- 
vity of all thefe, do depend. ‘upon the Qua- 
dratures of Curves; ‘tis plain, that thefe 
are eafily obtain’d too, if they depend upon 
the foremention’d Curves. 

After I had compos’d thefe Theorems, 
and fhewn them to the Celebrated Mr. New- 
ton, (as the fupream Judge in all Matters of 
this Nature) he was pleas’d to give me a 


_. fight of fome Papers of his, by which I find 


that he has a long time been Matter of a 
Method, by which any Trinomial &quation 
(exprefling the Nature of a Curve) being 
given, that Curve is either fquar’d, or re- 
duced to a more fimple one. 

And ’twere to be wifh’d, that he thought 
fit to communicate to the Publick, not only 
thofe Things which he has relating to thefe — 
Matters, but others alfo of his Noble In- 
ventions, which are not a fmall Number 
neither. And I believe this is not my With 
alone, but that of the whole Learned World 
befides. 

I make no queftion but thofe Learned Per- 
op (whofe een in the Ate Prudent 

ang 


158 Mifvellanea Curiofa. - 


and otherwhere, have tended fo much to the 


Advancement of Mathematicks) have Me- . 


thods nat unlike to this of mine; and there- 
fore I afcribe no more to my felf in this 
Matter, than only that I found out thefe 
Theorems, not knowing whether any Body 
elfe had done fo before or no; and reduced 
them into fo eafiea Form, that the whole 
Calculus relating to them, might be taken 


'. in, as it were, at one View. o 
But before 1° make an end of Writing, 


I think it improper, if (having not had an 
Opportunity fooner) I make fome little re- 
ply to the Famous Mr. Leibaitz’s Animad- 
verfions upon my Series for finding the Root 
of an Infinite Equation. 


That Excellent Perfon thinks fthis Series 


not to be General enough, as not reaching 
the Cafes where z and y are multiplied in- 


to one another; upon which account he 


fubftitutes another Series in the room of it, 


which he aflerts is infinitely more General. 


But that which led him into this fmall Mi- 
flake, I guefs to be this, that he took the 
Quantities a, b, c, d, &c. for given Quanti- 
ties, whereas they were to be us’d indiffe- 
rently, either for given or izdererminate ones. 

But I fhall add one Example to fhew that 
my Series extends to all Cafes. Let the 
Equation be zyz—<? =’. Beas ie 

In our Theorem let a=zy, b==0, c= —1, 


b=z0, s==1, or rather: let g=yy, hbo, eee. . 


| | Co) are, 
Then in either Cafe will <=—-+ —-++ — 


ray. a pam. iti ig? ‘ 


-|- teas wea eater &e. ° 
Ak ea Ny gn Tivo 


Maifcellanea Curio fa, BB 


Two Problems; viz. concerning 
the Solid of Leaft Refftance, 
and the Curve of Swifte/t De- 
foent. 

alv'd by J. Craig. 


LEMMA. 
Vy 'O find the Proportion between the Re- 
_ § fiftance made to the Rectangular Tri- 
angle AIG, and that made to the circum- 
fcrib’d Rectangle AlGg, while each moves in 
- a Fluid, in the direction of the Line IA, 
from I towards X. | 
From any point B let there be drawn BC 
perpendicular to AG, Bb parallel to Al, and 
BM perpendicular to AI. Then in bB take 
bH = CM? and bE= BC, and thro’ the 
| ota . 
‘points H and E, draw the Lines HA, EA, 
which being produced cut Gg in K and Ff. 
1 fay the Refiftance of the Triangle AIG 


_ is to the Refiftance of the Rectangle AlGg, 


as the Area of the Triangle AKG, to. 
the Area of the Triangle AFg. And 
alfo, that the Refiftance upon any part 
of the Line AG, 1s to the Refiftance 
upon the correfpondent patt of the Line 

| i. 7 Ag 


(160 = =©MaifceHanea Curiofa, 
Ag (ex. gr. upon AB and Ab) as the 
Area AHB to the Area AEB. The Demon- 
{tration of which depends upon a General | 
Theorem, which I deduced ey eafily from 
Prop. 35. haha P- 324. 


COROL, he 


_ Let BG, bg, be infinitely fmall parts of © 

the Lines AG, Ag, and let bB be produced 
to; Ll fay, that the Refiftance upon BG 
(which call e) is to the Refiftance mpon bg 
(which call E) as GL”: GB’. 

For e: E:: KHgb: FEgb; that is,e: E: 
bg x bH: bg x bE (by the foregoing Lemma ) 
therefore es E:: bH: bE s that is; €:'B: 
CM? : BC :: CM? : BC?. iat ea BC?:: 


GL? : GB? (becaufe of the fimilar Trian- 
gles BMC, GLB.) ‘Therefore e: EB: GL": 
GB’. Q: E:D. 


'GOROL. a8 F 


The Refiftance upon the infinitely fall _ 
part GB, is= GL’. For if all the infinite 


GB? 
ly finall parts in the Line Ag (as bg) be fup- 
pos’d equal, then the Refiftance upon bg, 
may be exprefs’d by bg, that is E=bg, ane. 
fo: E=GL: Therefore: (by Con. 1.8L: 
GL’: GB’, whence e= GL?. Qe Be. 


GB? 
COROL. 


Mifcellanea C uviofa: 1.01. 


So ROL? JH. 
Let r be the Radius, and c¢ the Circum- 
ference of any Circle. I. fay, that the Re- 
fiftance upon the Conick Surface generated 
by the Rotation of the Lineola GB about 
Al, is equal to the Product of cx BM into 


r 
GL’. For the Refiftance upon that Conick 
GB’ 


Surface, is equal to all the Refiftances upon 


the Lineola*GB, that is, to all thee; that 

is, equal to the Circumference of the Cir- 

cle (whofe Radius is BM) multiplied into-e ; 

that is, the Reffftance upon that Conick 
cx BM 


x e, and confe- 


: : cx BM GL? 
quently (by Coro/. 2.) equal to — x ) 


ae r GB. 


Surface, is equal to 
| : r 


PROB. IL 


To find a Curve Line, by the Rotation 
of which a Round Solid {hall be gene- 
vated, that, while ’tis moved in a Fluid 
Medium, in the Direction of its Axis, 
fball meet with the leaft Refiftance. 

(Fig. 24-) a 

Let OG, GB, be two infinitely {mall Par- 

ticles in the Curve fought, which rould a- 

bout its Axis, will produce the Solid of 
: | M leaft 


162  Mifcellanea Curwfa. 
leaft Refiftance. Draw BM, GP, perpendi- 


cular to AQ, alfo BL, GN, ‘parallel to oe . 
and ON, parallel to BM. — 


cx BM *.GL? 


. Now ais 5, Reales up. 
r x GB’ | 
on the Surface generated by the noe of 


Cy * GPx ON* 


the Lincola GBabout AQ, and : 
rx GO? 3 
is the Refiftancé upon the Sur yee generated 
OG, in like manner (by Cor®3.) And 
the Sum of both thefe Refiftances malts be 
a Minimum, vit. (we 
Cx Divi er cx GPx ON? 

-= a Mini- 


oe 


rx GB? : rx OG? 

YAU « : 
And confequently i in the Line RS (fo pa- 
rallel to AQ that ON—GL) the point G 
is to be fought, fuch, that this may happens, 
which, fuppofing the points O and B to be 
fix’d, will be eafily found by the common 
Method, de Maximis  Minmis. And pro- 
fecuting the Calculus, we fhall come at laft 
BM x BL . GPx NG 


; 


- to this. Equation, — 


, eBGt teas eee 
aM | BMx BL. | ms 
whence °tis plain that ——_ =a con- | 
BG* 


ftant ‘Ouantity: So that if the Abfeiffe 
AM = x, and the Ordinate BM=y, then’ 
will BL = dx, LG = dy (which I have fap-— 
ead "d 


Mifeelanea Cunibfe. a. 163 | 


: pos’d conftant every where in this. Calculus) 
and confequently BG* = dx’ -[- dy’, whence 
heist | 
deed ie dydy* 
be any conftant Quantity, and confequent- 
ly (to obferve the Law of Homogeneals) we 
ydx a 
have =, 
dxdx-\-dydy” — dy? 
by the Iluftrious 1 iii and the cele- 
| brated Fo. Bernoulli. 


aoa conftant Quantity. nee a 


ee os. I. 
te fina the poe of Swiftef Defcent. » 


(Fig. 25.) 

Let ‘BC, Ci, be 1 Sie infinitely fmall Par- 
ticles in the Curve fought. Now this Curve 
ought to be of fuch a Nature, that, fuppo- 
fing a Body to have' fallen from the Hori- 
zontal Line AQ, it may pafs from B to D 
in the fhorteft Time. Therefore we are to 
find out the Point C (in the Line RS drawn 
in fuch a manner parallel to AQ., that the 
differences of the Ordinates GC, DE, may 
be equal) fuch that this ey come to 


Batt. 

; Now the Veleeity in C is /LC, and that 
BC 

in D is /QD; therefore ——— is the Time 


M 2 ‘of 


(164 Mifcelanea Cuviofa. — 

- CD... | 
of Defcent thro? BC, —— is the Time of 
VQD 


Defcent thro? CD (by Prop. 54. pag. 158. 
Newt.) Therefore the point C ought to be 
BC | CD - 

VLE QD 
Suppofing ‘the points B and D to be fix’d, 
let the conftant Quantities GC=DE=m, 
LC=b, QD =p; the Indeterminate Quantities 
BG =u, CE =z; whence ' 


| Vn? tw? Vn Le ca Mi 


ith that 


may be a Atinimum. 


a/b Se 
@imum. Therefore. 
udu rae 
ee — 0. 


vbVme tut pV? 2? 
But du =—dz (becaufe y+ is conftant) 
therefore } 
u TNE, Le 


\ amt 
— 


5 whence ’tis 
Vb AY ig? but lp N/m? ie | i 


manifeft that — = a conftant 
VON me be 


Quantity. Now let the Abfcifle AL= 14 
the Ordinate LC=y, and to BG =dx, 
6: Bin ge “oe GG 


Ba 
ot 


— Maifcelanea Curiofa. 165 


GC =dy, BO=Vdx?+dy?, and let a 
be any conftant Quantity. Then hall 
aa Cee 


dy Vide? + dy? 
V dx? + dy?. - But now in all Curves, ’tis 


== —, whence dx Varivy x 


dw: Vax? +dy? :: as the Subtangent, to 
‘the Tangent. Therefore the Nature of the 
-Gurve fought is fach, that its Subtangent, 1s 
to the Tangent, as /:4/y, which that it is 
a Property of the Cycloid, is known to all, 
that know that the Tangent of the Cycloid, 
is parallel to the Chord of the Conterminal 

Arch, in the Generating Circle, whofe Dia- 
meter is 4, and whofe Vertex is downwards. 

‘And with the like eafe, I can find the 
Curve of the Smifteff Defcent, in any other 
Hypothefis of Gravity. 


M 32 T he 


166 Mifcellanea Curiofa. 


T be Quadratere of ihe Logarith- 


mical Curve. 


(Fig. 26.) 


By J. Caty. | 


ET ONF be the Logarithmical Curve, | 
whofe Afymptote is AR, in which let ; 


fach.a point A be taken, as that the firft 


Ordinate AO may be equal to the Subtan-— 


gent or Unity. ’Tis requir’d to find the 
Area of the Curvilineal Space AONM com- 
prehended under the two, Ordinates AO, 
MN, the Abfcifle AM, and the Curve ON. 
From. O draw OB, parallel to AM and cut- 
ting MN in £3 1 fay, that the Rectangle 
under the Segments ME, EN, is. equal to 
the Space pene, Demonhratiin.. Let” tie 
Ordinate MN =Z, Subtangent AO or ME 

m=s; and to the Axis AR let another Cutve 
HGE be conftructed, whofe Equation fhall 
_ he 2szx7, its Ordinate GM being =~. I 
fay, that this Curve is the Quadratix of the 


Lonanchenied Curve-(according to the Prin- 


ciples of my Method) wz. its Subnormal is 
refpectively equal to the Ordinate of this, 
as is plain from the Calculus of that Me- 
thod. " Therefore (according to what I have 
thewn in another place) if to the point G 
we draw GC perpendicular and equal toGM, 
as alfo HD parallel to GC, and meeting 
the Lines GM, cM, in B and D; then he 

the 


— Mifcellanea Curiofa. 167 
the TrapeziumGBDC = AONM. ButGBDC 
= GMG-— BMD = $x? ~;BM?= SZ— 
2 HAI; but HA = 2 AO? from the Nature 
of the Curve HGQ, therefore GBDC = SZ 
~ AO1= AOx MN — AOT= AOx MN— AO 
SMEx*x MN=ME=SMExEN. _ There- 
fore allo AODNM=MEx EN. Q:E-:D. 
When I applied my Method to thefe fort 
of Figures, I found that a Miftake had 
fome way or other crept into M. Bernoulh’s 
Calculus. For in his moft excellent Trac& 
of the Principles of the Differential Calculus, 
he affigns to the Figure whofe Equation is 
eS bse Ue. VDE yy 
ay, this for its Quadrature, vz. eer? 
a ae 
ie aad: 8 aly yy 
whereas the Area of that Figure 1s Re 
Ve eS BAR ae ae, ee 4a 
where y denotes the Abjfcifle and z the Or- 
dinate. we ; . , AY 


ei 
Ee IV OE 
cee oe ee Se 
. ‘ of Ps 
To Cah h J rey! § “8 
‘esi < ee ee 
teat Sa Bae : | : 
eat: ae ¥# es . 
| imi M ue AA 1 heos 
tert Don i ct) Sti 
Sagit 
vet ySe * 


168 . Mifclanea Oxted.  @ 


A Theorem concerning the Propor- — 
tion of the Time that a beavy 
Body [pends in defcending thro’ 
a right Laine joining two given 
Points, to the (fhorteft) Lame, 
in which it paffes from the one 

to the other of thefe Points, by 
the Arch of «a Cyclord. a 


THEO RE ae. 
(Fe. 29) 


N the Cycloid AVD, whofe Bafis AD is 
parallel to the Horizon, and the Vertex 

V turn’d downwards, if from A be drawn 
the right Line AB meeting the Cycloid in 
wny point as B, from whence is drawn BC 
perpendicular to the Curve of the Cycloid 
in B, and AC. be let fall perpendicular to 
BC from the point A: Then the Time that 
a Body at reft in A, fpends in defcending 
thro’ AB (by the force of its Gravity) 1s to 
the Time that it fpends in falling thro’ the 
Curve AVB, as AB to AC. {he ha 
Thro’ B draw BL parallel to the Axis of 
the Cycloid VE, and BK parallel to the Ba- 
_ fis AD, meeting the Axis in G, and the 
Circle (whofe Diameter is EV) in F and H, 
and the Cycloid gt felf in K: Draw the 


right: 


Mifcellanea Curiofa. 169 
right Line EF, which from the Nature of 
the Cycloid is parallel to BC; whence BM. 
is = EF, and EM= BF= the Arch VE 
from the Nature of the Cycloid , and ‘con- 
 fequently AM is = the Arch EHVF. 

By Propofition 25. Part Il. . Horolog. Ofcillat. 
Hugen. the Time in which a Body at reft 
in A defcribes the Cycloidal Arch AV, is 
to the Time of Defcent thro? EV, as the 
half Circumference to the Diameter. : 

And (by the laft Propofition of the fore- 
mention’d Part) the Time of Defcent thro’ 
VB, after the Defcent thro’? AV (which is 
equal to the Time of Defcent thro’ KV, 
i the Defcent thro’ AK) is to the Time 
of Defcent thro’ AV, as the Arch VF, to 
the Semicircumference ; and confequently to 
the Time of Defcent thro’ EV, as the Arch 
FV, tothe Diameter. Wherefore the Time 
of defcribing the Curve AVB, is to the 
Time of Defcent thro’? EV, as the Arch 
EHVF, tothe Diameter EV. But the Time 
of Defcent thro’ EV, is. to the Time of 
Defcent thro’? LB or EG, as EV to EF. 
Therefore (by Equality) the Time of de- 
fcribing AVB, is to the Time of Defcent 
‘thro’ LB, as the Arch EHVF, to the Sub- 
tenfe EF, that is, as AM to MB. Again, 
the Time of Defcent thro’ LB, is to the 
Time of Defcent thro’ AB, as LB to AB. 
Therefore the Time of defcribing AVB, 
is to the Time of Defcent thro’ AB, in the | 
Ratio compounded of AM to BM, and LB 
to BA, and confequently is equal to the 
 Ratioof AMx LB to MBx BA. ~ : 


But 


170 = Mifeellanea Curiofa. 
But AM x LB=MBx AC; and there- 


fore the Time in which a Body at reft in 
A, thal defcribe the Cycloidal Arch AVB, 
is to the Time of defcribing the right 
oe AB, as MB x AC to MBx BA; that 

> as AC to AB. Q: EB: Dis 

fans the Demonftration will pines in 
dike manner, if the point B be between A 
and a i 


: Mifcelanea Curiofa. | 17% 


An Extrait of a se eh from the 
Reverend Dr. John Wallis, to 
_ Richard Waller, E/q; Secretary 
to the Royal Society, concerning 


the Spaces in the Cycloid, which 
are perfectly Quadrable. | 


| Oxford, Aecae 22. 1695. 
sh8 Tuy. 
Find it is thought by moft, that there is 
no other part of the Semicycboid Figure _ 
- (adjacent to the Curve ) that is capable of 
being pepmetrically Squared, but thefe two, 
AR 
. The Segment AbV, (Fig. 28.) taking 
A pee = Aa, (which was. firft obferv’d. by 


Sir Chriftopher Wren, and after him by Huge- 
nivs and others) and it is = 43 Key R* 


3° 
¥ as 1 Des Trilinear 4 dD (taking dD, in 
the Parallel d DC, pafling through the Cen- 
ter C,) which is = R?. 
. But, it is otherwife (as I have fhewed in 


my Treatife, De Cycloide, and that, De Motu ; 


x the Figures of which latter I retain here, 
fas far as they. concern this Occafion ) there 
. | being 


172 4 Maifcellanea Curiofa. — 
being other Portions of it, equally capable 
of Quadrature. 

In order to which, I there fhew (De AZotu, 
Cap. 5. Prop. 20. A. p.802,803,804-) that not 
only the Cycloid is Triple to the Circle Ge- 
nerant, (which was known before) but that 
the re/pective Parts of that are Triple to thofe 
of this: Which is the Foundation on which 
I build my whole Procefs concerning the Cy- 
claid in both Treatifes, (and which is not pre- 
tended, that I know of, to have been obferv’d 
or known by any Body before me:) That is, 
bpaA (Fig.28.) Triple to the Seftor Ba A 
(taking 6g parallel to Ba) where-ever, in 
the Curve 47+, we take the point 6. 

1 then fhew, that the Cycloid ts a Figure 
compounded of thefe two; the Semicircle 
A Da, and the Trilinear A Darb A, lying 
between the two Curves 4D. and Adz, 
(and therefore, to Square any part of thefe, 
is the fame as to Square the refpective part 
of the Cycloid. 

I fhew farther (Jbidem, pag. 804.) that this 
Trilinear is but a diftorted Figure (by rea- 
fon of the Semicircle thruft in between it 
and its Axis) which being reftored to its due 
Pofition (by taking out the Semicircle into 
a different Figure, (as Fig. 29.) and thrufting 
the Lines 6B home to the Axis, fo as that 
BV be the fame point) is the fame with 
Ara, (Fig. 30.) (the Parallelograms bf 4B 
being fet upright, which in the Cycloid ftand © 
floping; and the Circular Arches 6 2, (Fig. 28.) 
becoming ftreight Lines (in Fig. 30.) and the 
‘Lines 6 B being, in both, equal to the refpe- 

| ctive | 


: Mifcellanea Curiofa. 173 
étive Arches B A, every where ;) which there- 
fore I call Trilineum Reftitutum (the Trilinear . 
reftored to its due Pofition, which Figure I 
do not find that any before me has confi- | 
der’d: ) So that to Square any part of this, 
is the. fame as to Square the refpedctive part 
of the Cycloid, (or of the Trilinear in the 
Cycloid: ) That which in the Cycloid lies be- 
tween two Aiches of the Circle Generant 
in different Pofitions, anfwering to that 
which, in the reftored Figure, lies between 
the refpective ftreight Lines. 

And therefore 4d D A, =7d 37, (Fig.28.) 
= Aa DA pr, (Fic. 30.) = R*. And 
AbkdA, rbk dr, (Fig. 28.) = Abkd A, 
Tbk S7, (Fig.30.) —sR. And bk.d (Fig.28.) 
= bkd, (Fig. 30.) == R? — sR, Ibid. Cap.17. 
B. pag. 756. Where, if 6 be taken above 

dak DC, (pafling through the Center C) thefe 
Figures are within the Cycloid, and within 
the reftored Figure; but without them, if 


___b be taken below that Line, and adjacent to 


the Curve 467, in both Cafes. 
By R, I underftand the Radius of the Cir-- 
cle Generant; and by s, the Right Sine of 


the Arch B 4, whofe verfed Sine is VA. 


And, where-ever in my whole Difcourfe 
of the Cycloid, or the reftored Trilinear 
(which is a Figure of Arches, and a Figure 
of verfed Sines) the Arch 2 is no Ingredient 
in the-defignation; fuch part or portion of 

them is capable of being Geometrically 

fquared. But when I exclude a, I do there- 

in exclude P (for that is an Arch alfo) and 

f=a-+s,ande=—2—s, becaufe a is theres 
in included. 

: Mr. 


174, Mzfcellanea Curiofa. ! 
Mr. Cafmell, (not being aware that I had 
fquared thefe Figures) had done the fame by | 
a Method of his own, (which he fhewed me 
, lately) which I would have inferted here, 
but that he thought it not’ necéflary; and 
inftead thereof, hath given me the Quadra- 
ture of a Portion of the Epscycloid (which 
you will receive with this) and, I think, it 
is purely new. 


Mifcellanca Curiofa.. 175 


The Quadrature of a Portion of 
the Epicycloid. Se, GUO 
aa — By Mr. Cafwell. 


(Fig. 31.) 

Supe DPF to be half of an exterior 
De Epicycloid, 7 B its Axis, Y the Vertex, 

VL B half of the Generant Circle, E£ its 
Center; DS the Bafe, C its Center: Bi- 
fe& the Arc of the Semicircle Y B in Z, and 
on the Center C through Z draw a Circle 
cutting the Epicycloid in P: Then I fay the 
Curvilinear Triangle YL P will be= BEq 


in ae that is, the Square of the Semidia- 


meter of the Generant Circle will be to the 
Curvilinear Triangle Y LT, as CB the Se- 
midiameter of the Bafe, to CE; which CE. 
in the exterior Epicycloid is the Sum of the 
Semidiameters of the Bafe and Generant, 
but in the interior Epicycloid Dp, ’tis the 
difference of the faid Semidiameters. 


COROLLARY. 


In the interior Epicycloid, if CE is } CB, 
the Epicycloid then degenerating intoa right . 
Line, the Quadrature of the Triangle / xp 
will be in effect the fame with the Quadrature 


of Hippocrates Chins. 
| | CORUL. : 


Se RE: Oe hn a eee 
TAY ye Fas soars 
, id r ‘ 
bbe, 


176: Mifcellanea Curiofa. ane 


COROL. IL 


Bri 
i 


If the Semidiameter of the Bafe is fuppofed 


infinite, the Epicycloid then being the com- 
mon Cycloid, the Area of the faid Triangle 
will be equal to the Square of the Radius of 


the Generant, and fo it falls in with that — 
Theorem which Lalovera found, and calls 


Mirabile. | “se : 
Though I do not think the abovefaid Qua- 
drature can eafily be deduced from what has 
been yet publifhed of the Epicycloid, I have 
not added the Demonftration; but think it 
enough to name a general Propofition from 
whence I deduced it, viz. The Segments of 


the Generant Circle are to the Correfpondent 
Segments of the Epicycloid, as CB to 2CE 


-+-CB. For Example, fuppofe Fm G the 
Pofition of part of the Generant when the 


point F of the exterior Cycloid was defign’d, 


then the Segment Fm G x is to the Segment 
DFuG::asCBto2CE-|-CB. 


And confequently the whole Epicycloid to 


the whole Generant in the fame Proportion: — 


Which is the only Cafe demonftrated by 
Moufieur De /a Hire. : 
It follows alfo that inthe Vulgar Cycloid, 
its Segments are triple of the Correfpon- 
dent Sectors of the Generant, which. was 
firgt Shewn-by Dr. Wallise. cee es 


A General 


ee I Fe, ee ar Pome, AS se t 
Ape eae PSIG ae Ue 3 ¥ 


2 ‘s Mifeellanea Curriofa. oe 77 


* 


| A General Propofition bering the 


— Dunenfion of the Areas in all 
thofe kinds of Curves which are 
deferib'd by the Equatle Re- 
_volution of a Circle upon any | 
| Bafis, evther a Rectilineal or a 

— Circular one. | 


BTS 24 By Edm. Halley. 


SFP VIS known that the Primary Cycloid, 


= # as alfo the Prolate, and. the Contratted 


-one (which they call Trochoids) have been 
. largely: handled by the Celebrated Dr. Wai- 


_ lis and others, and their Properties are now 


common enough ; fo that there’s fcarce. any 
thing new left to be difcover’d concerning 


them. But the famous M. De Lattire in a 


late Treatife, having fhewn fome of the Pro- 
perties of the Primary Epicycloid, the moft 


‘Ingenious Mr. Ca/mell did upon that occafion 
not: only demonftrate that the Menfuration ~ 


of the whole Epicycloidal Space, obtain’d al- 


-fo in the parts of the faine, but alfo gave 


a perfec Quadrature of the Curvilineal Space 


UPL. But while I was enquiring after the 


Demonftration of this Quadrature, which is 


“pot very obvious, nor as yet given by the In- 
 yentour, I light upon the following general 


Pro- 


ed x 


178 Mifcellanea Curwfa. 

Propofition, by the help of which all forts of 
Curvilineal Spaces, as well of the Cycloidal 
as Epicycloidal kind, as well the whole 
Spaces as the parts, are meafur’d. And far- 
ther, not only the Spaces VPL, but alfo in- 
numerable others, QTP and VQOTL, are de- — 
monftrated to be capable of an exact Qua- . 
drature; and this not only in the Pramary 
Epicycloids, but but alfoin the Prolare and 
contracted ones. By kes 

The Prupofition is as follows. 


Propofition. , 

The Area of any Cycloid or Epicycloid, 
either Primary, Prolate, or Contraéted, is 
to the Area of the Generating Circle, and — 
alfo the Areas of .the generated parts in 
thofe Curves, are to the Areas of the Ana- 
logous Segments of the Circle; as the Sum 
of twice the Velocity of the Center, and — 
the Velocity of the Circular Motion, to the 
Velocity of the Circular Motion. , 


Demonfiration, * — 


be (Fig. 32.) 

Let YPQRSUB be any Epicycloid defcrib’d 
by the Revolution of the Circle ULB, up- 
on the Circular Bafis YMINB. Let the Cen-. 
ter of the Generating Circle be in ¢, and 
drawing cMK, let the Circle ftand upon the — 
Bafis in the point M, and let the defcribing — 
point be S. Now diftinguifhing the Motions, 
Jet the point S firit of all be carried by the — 
Circular Motion into R, fo that the Arch 


| MifceHanea Curtofa. 17979 - 
SM is increafed by the indivifible Particle | 
RS. Next fuppofe the Center c to be tranf- 
ferr’d to C; by which Motion the Segment. 
RSM being brought into the Pofition QTN, 
_the point Q will touch the Curve. ’Tis 
plain that the Triangle RSM is the Mo- 
mentum or Fluxion of the Segment of the 
Circle, and that the Trapezium QSMN is 
the Fluxion of the Curvilineal Space gene- 
rated in the fame time. And fince SM, 
RM, QM, are fuppos’d to differ but by a 
pont from one another, let the little Area 
QSMN be conceiv’d to confift of the three 
Sectors RMS, RMQ, MQN; and fo the 
little Area RMS to be to the little Area 
_QSMIN, as the Angle RSM to the Sum of the . 
_ three Angles RMS-|-RMQ-|-MQN. But the 
AnglesRMQ-|- MON, are equal to the Angles 
MCN -- MEN, or to the Angle cMC ; be- 
-caufe of the Lines RM, QN, inclin’d to one | 
egret ‘in an Angle equal to MKN, and 
becanfe of the Angle MQN equal to ] MCN 
(by Excl. 3. 20.) confequently the Angle 
RMS is to the Angles RMS-|+-cMC, that 
As (by the fame Propofition mention’d) the 
Arch 3 RS to the two Arches Cc-+-3 RS, or | 
RS to 2Cc IRS, as the little Area RSM, 
‘to the little Area QSMN, or as the Mo- 
mentum of the Circular Segment QTN, to 
the Momentum of the Epicycloidal Segment 
OSYMN generated in the fame time. And 
ce thefe Momenta are ever in that fame 
Ratio, where-ever the point Q_ be taken, ’tis 
Manifeft that the Areas QTN, QSMYN 
themfelves, generated from thefe Momenta, 
Thave alfo the fame conftant Ratio, viz. - 
oc N 2 tne 


i180 = Mazfcellanea Curiofa. 

the Velocity of the Circular Motion RS, to 
double the Velocity of the Center, adding 
the Circular Motion, or 2Cce-| RS: As al- 
fo the Area UBZ to the Area QUBN, and 
confequently the Semicircle ULB to the Cur- 
vilineal Space UQYNB.. Wherefore the 
Propofition is manifeft. | | 

And there is no other difference in the 
manner of demonftrating, if the generating 
Circle moves upon the Concave fide. of the 
Arch, except only that the Angle cMC, in 
this cafe, is the difference of the Angles. 
MCN, MEN. But if the Bafis were a right 
Line, then MKN vanifhing, and RM, QN, 
being parallel, the Conftrudion will be ea- 
fier. 1 forbear drawing Corollaries from this 
Propofition, fince they are obvious. But 
now in all thefe Curves, the Portions that 
are Analogous to thofe Portions which Do- 
ctor Wallis has found capable of a perfect 
Quadrature in the Primary Cycloid, are here 
alfo equally fquarable; which eafily follows 
from what has been faid. 

Upon the Center K, thro’ the point Q., 
draw the Circular Arch QZ, and draw ZB 
cutting off the Segment ZLB = the Segment 
- QTN.. Then bifecét the Semicircle UB in L, 
and thro’ the point L and on the Center K, 
defcribe the Arch PL cutting the Epicycloid 
in P, the generating Circle in T, and the 
Chords QN, ZB, in y and X. Let the Arch 
VZ.= a, its Sine =, the Radius of the 
generating Circle = r, the Radius of the 
-Bafe=R, and the Arch CE or the Motion 
of the Center =m. It is plain that the 
Sector CKE, is to the Space XyINB, as the 

| | © ~~ Square 


——, Mifeeltanea Curtofa. 18% 
Square of KE, to the difference of the 
- ‘Squares of KL and KB, or asRR-l 2Re-brr, 
fae a 201, chat is, as R.F t,.to 2r, or 
KE to BV. And confequently the Rectan- 
gle BE. x CE or rm is equal to the Space 
XyNB. But the Space VZB is equal to the 
‘Rectangle 3 ar 13 sr, and. fo according to 
our Propofition it will be as 4 to 2m, fo } ar 
ee May is, 7 ay 
“S sr, to SL ae equal to the Curvilineal 
Space QUZLBNQ: From hence fubftra& 
the Space XyNB==rm, and there remains 
the. Space QUZXy ==. And fince the 

‘Spaces ZXL, QyT, are equal, the Space 


QULTQ. fhall alfo be equal to ae ed ficre- 


fore when ato m, or the Circular Motion 
is to the Progreflive Motion of the Center, 
‘in a given Ratio, there will be a perfec 
Quadrature of the Curvilineal Spaces 
~QULTQ. And the whole Space UPL, will 
_ be to the Square of the Radius BE, in the 
fame Ratio (m toa) of the Motions, that 
is in-every Primary Epicyclotd;-in-the Pro- 
portion of the Radii, KE, KB, which is 
Mr. Cafwell’s Propofition. 

But the leffler Spaces QULTQ will be to 
- one another, as the Sines of the Arches UZ; 
and the Triangular Spaces QTP, by the fame 
Argument, will be as the verfed Sines of the 
‘Arches QT or ZL, and confequently are al- 
fo fquar'd. After the fame manner it will 
be prov’d, that the Spaces par, pLu, par, 
are ever to the Square of the Radius BE 
N 3 mete 


782 0 )©=— Mifcellanea Cueiie one 


Cin all thefe Figures) in the aforefaid Ratio 
of m toa; and their Portions pqt, as the 
verfed Sines of the intercepted Arches qt; 
but the remaining Segments as qtYA,. qtTa, &c. 
will be as the right Sines of the Compli- 
ments of the fame Arches 5 ag 

But the Ratio of the Velocities, m tO 4, is 
compounded of the Ratio of the Radii KB, : 
BE, and the Ratio of the Angles ~ CKE, 
VEZ, equably defcrib’d together; and con- - 
fequently giving that Ratio of the Angles, 
all the foremention’d Epicycloidal Spaces 
will be fquar’d alfo. : 

I can eafily draw Tangents to all thefe 
Curves, as alfo I feem to my felf to have 
gotten their Reifications, from fome Areas 
Analogous to. them ; which may give occa- 
fion_ to a more particular handling of as 
Family of Curves another time. | : 


Mifcellanea Curiofa. 883 


A Method of R.aifing an infinite 
Multinomial to any given Power, 
or Extracting any given Root of 

the fame. fe ES 
_. By Mr. A. De Moivre: 


_ 9F PIS about two Years fince, that confi- 
-°§ dering Mr. Newtons Theorem for 
Railing a Binomial to any given Power, or 
Extracting any Root of the fame; I enquir’d, 
whether what he had done: for a Binomial, 
could not be done for an infinite Multino- 
mial. I foon found the thing was poffible, 
_and effected it, as.you may fee in the follow- 
ing Paper; I defign ina little time to fhew 
the Ufes it may be applied to: In the mean 
while, thofe that are already vers’d in the — 
Doérine of Infinite Series, and have feen 
what Applications Mr. Newton has made of 
his, Theorem,.may of themfelves derive fe- 
veral Ufes from this. : 
I fappofe that the Infinite Number Multi- 
Momial sig 1 bez \ cz? | dz* en”, ec. m 
is the Index of the Power, to which ‘this 
Maltinomial ought to’ be Rais’d, or if you 
Will, "tis the Index of ‘thé Root which is to 
be Bxtiadedy I fay that this Power or Root 
of'the Multifomial,\ is fach a Series as | 
Bh e@iarcieit iss yd obi buss ye vig 
“Bhieao! N 4. For 


184 Mifcellanea Curiofa. 

For the underftanding of it, it is only ne- 
ceflary to confider all the Terms by which 
the famé Power of z is multiplied, 1m or- 
der thereto I diftinguifh two things in each — 
of thefe Terms; Firft, The Product of cer- 
‘tain Powers of the Quantities, 4, 6, ¢, d, Xc- 
Secondly, The Uncia (as Oughtred calls em) 
prefixt to thefe Produéts. To find’ all the 
- Produéts belonging to the fame Power of z, 
to that Produét, for inftance, whofe Index ts 
mr (where ry may denote any integer Num- 
ber) I divide thefe Products into feveral Claf- 
fes; thofe which immediately after fome 
certain Power of 2 (by which all thefe Pro- — 
du€&ts begin)! have 6, I call Produéts of the 
fir Claffis; Bor Example, a™—~* be is a Pro- 
du@ of the fir Cla/fis, becaufe 6 immediate- 
ly follows 2”—*3 thofe which immediately 
after fome Power of a have c, I call Products — 
of the fecond Cla/fix, fo a2”? ced is. a Produc ~ 
of the fecond Claffis, thofe which immedi- 
ately after fome Power of a.have 4, | call 
Enos of the third Cla/fis, and fo of the 
reit. 7 | AES Ween 

This being done, 1 multiplyall the Products 


\Wa 


by @ all the Terms, be+ 
Es ae 


Mifcellanea Curiofa.  ¥8g 
longing to z mrr—4_ except thofe of the firft, 
fecond, and third Claffis, and fo on, till i 
meet twice with the fame Term. Laftly, I 
add to all thefe Terms the Product of a”—" 
into the Letter whofe Exponent is r--1 

“Here I muft take notice that by the Ex- 
ponent of a Letter, I mean the Number 
which expreffes what Place the Letter has in 
the Alphabet, fo three is the Exponent of 
fie etter: ¢ * becaute.' the Cetter. ¢ is the 
third in the Alphabet. 

‘At is evident that by this Rule. you may 
ait find all the Produéts belonging to the 
feveral Powers of z, if you have but the Pro- 
dud belonging to 2” viz. a™ 

To find the Uzcie which ought to be pre- 
fixt. to every Product, 1 confider. the Sum of 
Units contain’d in the Indices of the Let- 
ters which compofe it (the Index of a ex~ 
cepted) I write as many Terms of the Series 

mrm—-1x%*m—2x m—3,&c. as there are 
Units in the Sum of thefe Indices, this Series 
is to be the Numerator of a Fraction, whofe 
Denominator is the Produé of the. feveral Se- 
ries TR2% 3X4 % 55,06 1X 243 e.4X.5., oc, 
TX2KX3%4%5X%6, &e. the firf€ of which 
contains as many Terms as there are Uvits in 
the Index of b, the fecond as many as there 
are Units in the Index ‘of c, the third as ma- 
“hy as there are Vuiets in the Index of d, the 


fourth as many as there are Units in the Index 
of e, &e. eye é 


De. 


& 
©. 
FS 


a 


186 Mifcellanea Curiofa. — 


Demonftration. 


To raife the Series az -|-bzz--ez3 + dz*,&e. 
to any Power whatfoever, write fo many Se- 
ries equal to it as there are Umits in the In- 
dex of the Power demanded. Now it Is evi- 
dent that when thefe Series are fo multipli- 
ed, there are feveral Products in which there. 
is the fame Power of z, thus if. the Series 
ez tbe 4 cz). tdz*, | &c.. iss raed 4048s 
Cube, you have the Produds 6°z°%, abez®, 
aadz®, in which you find the fame Power z° 
Therefore let us confider what 1s the Condi- 
tion that can make fome Prodads to contain 
rhé fame Power of z, the firft thing that will 
appear in relation to it, is that in any Pro- 
duct whatfoever, the Index of z is the Sum 
of the particular Indices of z in the multi- 
- plying Terms (this follows from the Nature 
of Indices) thus 632° is the Produ@ of bz?, 
b27, bz?, andthe Sum of the Indices in the 
multiplying Terms, is 2-2‘ + 2&6 sabes 
in the Prodad& of az, bzz, cz3, and the Sum 
of ‘them “Indices of z‘in the multiplying 
Terms is 174-2136 aadz® is the Produd& 
of az, az, dz*, and the Sum of the Indices 
of 2 in'the multiplying Terms is 1-+it4=6; 
the’ next thing’ that appears is, thatthe In- 
dex of x in the multiplying Terms is the 
“fame with the’ Exponeiit © oF the Letter to — 
to which z is join’d, from which two Confi- 
derations it follows, that, To have all the Pro- 
ducts belonging to a certain Power of 7, you muff 
find all the Produtts where the Suna of the Ex- 

HE ; _ pouents — 


- 


Mifcellanea Curiofa. 1 87 
ponents of the Letters which compofe ’em fhall 
always be the fame with the Index of that Power. 
Now this is the Method I ufé to find eafily 
all the Products belonging to the fame Pow~ 
er of z, Let m-|-r be the Index of that 
Power, I confider that the Sum of thé Ex- 
ponents of the Letters which compofe thefe 
Produéts muft exceed by one thofe which be- 


long to m™1’—", now becaufe the Excefs of 
the Exponent of the Letter b above the Ex- 
ponent of the Letter 4, is one, it follows 
that if each of. the Produéts belonging. to 
z\7—! is multiplied by 6, and divided by 4, 
you will have Products the Sum of whofe Ex- 
ponents will be #-|-r;, Likewife the Sum of 
the Exponents of the Letters which com- 
pofe the Products belonging to z™I™ exceeds 
‘by two the Sum of the Exponents of the 
Letters which compofe the Products belong- 


ing to z™!’—?; Now becaufe the Exponent 
of the Letter a is lefs by two than the Ex- 
ponent of the Letter c, it follows, that if 
each Produét belonging to zmtt—2 is multic 
plied by ¢ and divided by 4, you will have 
other Products, the Sum of whofe Exponents 
is till m-lr; Now if all the Products be- 
longing to zit1—2 were multiplied by ¢ and 
~ divided by 2, you would have fome Produds. 
that would be the fame as fome of thofe 
found before, therefore you muft except out 
ef em thofe that I have’ call’d Produ&s of 
the firft Claffis; what I have faid fhows why © 
all the Products belonging to hig Sd so 
cept thofe of the firft and fecond Cla/fis pa 


188 Mifcellanen Curiafa. | 


~ 


Letters of each Solid may ‘be changed. 


be multiplied by d and divided by 4:, Laftly 
you fee the Reafon why to all thefe Products 
is added the Produ@ of a”—" by. the Let- 
ter, whofe Exponent. is rl 14 "Tis becaufe 
the Sum of the Exponents is ftilla-r. © 


As for what relates to the Unciaz;, obferve 
that when you multiply 2z-bzz }-cez3 4-dz*, 
&c. by ax bzz ez} -- dz*, &c. each Let- 
ter: 4)°b,) co; d> &e. ofthe Tetone semes i 
multiplied by each of the Letters 2, 6, c,d, 
&c. of the firft Series; Thus the Letter 2 of 


_ the fecond Series is multiplied by the Letter 


& of the firft, and the Letter_d of: the: fe- 
cond Series is multiplied by the Letter a of 
the firft; therefore you ‘have the: two Planes, 
ab, ab or 2ab for the fame-reafon you have 
2ac, 2ad, &c.,. Yherefore you muft prefix to 
each Plane of thofe that, compofe the Square 
of the infinite Series az-\ bez-\ez3, &e, 
the Number which exprefles\how many ways 
the Letters of each Plane may be. changed; 
likewife if you multiply the Produd of the 
two preceeding Seriés by az-bzz*}ex3, &c. 
each Lettera; 6; ¢, dj ofthe third ‘Series is 


multiplied by each of the Planes form’d by 


the Produét of the® firft and fecond Series; 
Thus the Letterzis multiplied by the Planes - 
bc and.ob;.the,Letter @ is multiplied, bya 
and ca; the Letter.¢,is multiplied by. and 
ba, therefore yous have, the fix. Solids;, abe; 
ath, bat, bea, cub, cha, or Sabe ;:, Therefore 
you, muft» prefix. to;cach Solid whereof the 
Cube of the infinite Series :is compos’d, the 
Number which expreffes haw. many ways aps 

| FAs 


, genes ~ 


| Mifcellanea Curiofa. 4 89 
generally, You muft prefix to any Produ where- 
of any Power of the infinite Series az bzz-- 
cz>, &c. w composed the Number which expref- 
_fes how many ways the Letters of each Produ& 
may be changed. | 


Now to find how many ways the Letters 
of any Product, for inftances a”—” bc? at 
may be changed; this is the Rule which is 
commonly given: Write as many Terms of 
the Series 1% 2%3% 4x95, &c. as there are 
Units in the Sum ofthe Indices, wz. m-2 
th-p-r, let this Series be the Numera- 
tor of-a Fraction whofe Denominator fhall 
be the Produét of the Series 1 x 2x 3% 4% §, 
ee O28 2h 4X54 Ce. 1X 2X 3X'4% 8X6, * 
&c. 1X 2% 3x%4x 5, &c. whereof the firft is 
to contain as many Terms, as there are 
Units. in the firft Index m—x; the fecond 
as many as there are Units in the fecond In- 
~ dex 43 the third as many as there are Units 
in the third Index p;_ the fourth as many as 
there are Units in the fourth Indexs;y. But 
the Numerator and Denominator of this 
Fraction have a common Divifor, wz. the 
Series 1x 2%3x%4%x5, &c. continued to fo 
many Terms as there are Units in the firft 
Index m—2; therefore let both this Nume- 
rator and Denominator be divided by this _ 
common Divifor, then this new Numerator 
will begin with m~x#-\1, whereas t’other 
began with 1, and will contain fo many Terms 
as there are Units in b-+p-\r, that is, fo 
many as there are Units in the Sum of all 
the Indices, excepting the firft; as for the 
new Denominator, it will be the slurs of 

. three 


_ 


190 =6§ Mifcellanea Curtofa. 
three Series only, that is, of fo many as their 
Indices, excepting the firft. But if it hap- 
pens withal, that 2 be equal to h-t-p-r as 
it always happens in our Theorem, then the 
Numerator beginning by m—x-\.1, and be- 
ing continued.to fo many Terms as there are 
Units in b‘\ p-\r or 2, the laft Term will be 
m neceflarily, fo if you invert the Series and. 
make that the firft Term which was the laft, © 
the Numerator will be mxm—txm—z2 
x m—3, &c. continued to fo many Terms 
as there are Units in the Sum of the Indices 
of cach Produét, exceping the firft-Index. 
There remains but one thing to demontftrate, 
which is, that, what I have faid of Powers 
whofe Index is an Integer, may be adapted 
to Roots, or Powers whofe Index is a Fra- 
ction; but it appears at firft fight why it. 
fhould be fo: For, the fame Reafon which 
makes me confider Roots under the Notion 
of Powers, will make me conclude, that what- 
ever is faid of one may be faid of tother ; 
however, I think fometime to give a more 
formal Demonftration of it. . ised 


SS sarees acy See 


LTRCOTEM. 


a Sd 
ae+hz? +c27 + dz*+ezi+fz2° + 9Z7 + Az? + 429 KC. 


Page Lg 27 


72 


a 


72 


Z 


Me jy TL M2» WL 7 W—-2 


pm n”’~d 


w 


+z x 22 y Fe? « -3 a Meat al 


+ fix Minty mma QQ” 3 Pd 


MAR 2 2 
+Brmee ac + Be ttn tee 29 be? 
BES w— Z 
age e é +3 xB gag”? be 
eg ea a Ce 
m—L 
+poan f 
t 


( = 7 22 od 
AP x Meaty Peay Me 1 Mey Bian 8 pp te MER hee 
e 
+ ¢ Mik y WB y 3 x mt = he 
+ Fx Mipty moag mes a™—* Yd 


x Mga y Many med g™-# fica 


+7 
PRX Baty m2 Qe? be 


Hee, wea 2 hed 


RR ARE 


= 2 2 2 m3 m+ 
4 ma MAG gt 4 Bey reg gfe MAA 4 my moty 2g 3 hig 3 


PP iar tpt, Baa" "be" 4 my mes mary mee ghee tS 


+H x Bbptx Manz 2"? HM ¢ 


se N 


j 2 
oh ae 
4 


ty eal 


So tes Seiichi Lovanbod a bl 
ai i a is mca: 


Ho ee aa 


Py teotnnhe y= nah aot iin 
: ’ 


j. 
A ed 


1 oe 
pene, § 
§ 


. ‘ Lig encima time a 


ek yi - ¥ 
i Sere 
Oe) oe plete tn eosin Sacs ss os Sey lta PONT 
Fe j 
Wid , 
? 


= doce 
siewaaign 
aah. 


CUM 
RR Hea ACN 


Maifcellanea Curiofa. 191 | 


A Method if eee a the Root 


mi an Infinite Equation. 
By A. De Moivre, ERS. 


THEOREM. 
Pu arbarperstdet fort f°, &e. = gy! 
“thyyrry? ee Ai -+my®, &c. then will 


z be o£ fy 


ir 
“ 


a 
io) ul = cA} 
ay? 
ied 
ke bBB—2bAC— 3¢ AAB = dAt 
eee , ——y* 
a 
1—2bBC—2bAD—3 c ABB—3¢ AAC—sd A> B 
—eA? 
OEE ee ys 


i 


Bt morr 


m =--2 BD --- bCC---2)_AE --- cB} --- 6c. ABC 
won 3¢- AAD == 6A AABB---41 A} C---52.A*B 
menhite 


ena meena einer 


y°, &e. 


a 


For the underftanding of this Series, and oe ‘ 


“in order to continue it as far as we pleafe, 


it is to be obferv’d, 1. That every Capital 


p Letter: is equal to the Coefficient of each 
pre- 


192  Mifcelanea Curiofa.. 
preceding Term ; thus the Letter B is equal to 


the Coefficient h—bA A 


2. That the De- 


nominator of each Coefficient is always a. 
3. That the firlt. Member of each Numera- 
tor, is always a Coefficient of the Series 
gy--hyy-iy?, &e. viz. the firft Numerator 
begins with the firft Coefficient g, the fecond — 
Numerator with the fecond Coefficient 4; 
aud fo on. 4 That in every Member after 
the firft, the Sum of the Exponents of the 
Capital Letters, is always equal to the 
Index of the Power to which this Member 
belongs: Thus confidering the Coefficient ~ 


pulser ee —— bes 4 9 
pic laleDRcirano NE cee ; which be- 


longs to the Power y*, we fhall fee that in 
every Member bBB, 2b:AC, 3CAAB, 4A*,. 
the Sum of the Exponents of the Capital. 
Letters is 4, (where I muft take notice, tliat” 
by the Exponent of a Letter, I mean the 
Number which expreffes what Place it has in 
the Alphabet ; thus 4 is the Exponent: of the 
Letter D) hence I derive this Rule for find-. 
_ ing the Capital Letters of all the Members 
that belong to-any Power 5 Combine the Capi-— 
tal Letters as often as you can-make the Sum ‘of 
their Exponents equal to the Index of the Power to 
which they-belong. §. That-the Exponents of | 
the fmall Letters, which are written before 
the Capitals, exprefs how many Capitals 
there is in each Member. 6. That the Nu-~ 
merical Figures or Uvese that occur in thefe » 
Members, exprefs the Number of -Permuta-. 
159 TIONS 


‘ 


, Mifceilanea Curiofa. . 192 
tions which the Capital Letters of every 
_ Member are capable of. | | 
_ For the Demonftration of this; fuppofe 
= Ay- Byy-|-Cy3-|-Dy*, &c.  Subftitute this 
‘Series in the room of z, and the Powers of 
_ this Series, in the room of the Powers of <3 
there will arife a new Series, then take the 
Coefficients which belong to the feveral 
Powers of y, in this new Series, and make 
them equal to the correfponding Coefficients 
of the Series gy-|-hyy-|-zy3, &c. and the Co- | 
efficients 4, B,C, D, &c. will be found fuch - 
vas I have determin’d them. 
But if any one defires to be fatisfied, that 
the Law by which the Coefficients are form’d, 
will always hold, P’ll defire em to have re- 
courfe to the Theorem I have given for. rai- — 
fing an infinite Series to any Power, or ex- 
tracting any Root of the fame; for if they 
ee ufe of it, for taking fucceflively the 
Powers of <Ay-\-Byy-|-Cy?, &c. they will fee © 
‘that it muft of neceflity be fo. I might have 
made the Theorem I give here, much more 
‘General than it is; for I might have fuppos’d, 
abe) ge a ai [2 res f opm oy by 3 -|- ails 
‘&c. then all the Powers of the Series .4y-|- 
Byy-\-Cy? ,&c. defign’d by the univerfal Indices, 
‘Mmuft have been taken. fucceflively ; but thofe 
who will pleafe to try this, may eafily do it, 
Dy means of the Theorem for raifing an infinite 
Series to. any Power, &c. 
\This Theorem may be applied to what is 
called the Reverfion of Series, fuch as find- 
Ing the Number from.its Logarithm given; 
the Sine from the Arc; the Ordinate of an 


. en 


Rage 3 A 18a toe c ao Rua tS ERMe eit 
ata Aes 


194  Mifcellanea Curwfa. : 
Ellipfe from an Area given to be cut from | 
any Point in the Axis: But to make a pat- — 
ticular Application of it, Pil fappofe we have — 
this Problem to folve; vz. The Chord of 
an Arc being given, to find the Chord of © 
another Arc, that fhall be to the firft as 
“ to 1. Let y be the Chord given, % the 
Chord required ; now the Arc belonging, to— 
cos he 
we Chontyy is) ¥ ++ 6dd a 4oa* is 112a°— 
&c. and the Arc belonging to the Chord hi 
eos i oge) an SBE arft of 
a -|- sod! BPS Flic the firft of 
thefe Arcs is to the fecond as_1 to 73 
therefore multiplying the Extreams and 
Means together, we fhall have this Equa- 
tion: : ic 
12) 3) ee 
64a god" ae one be, be 7) odd 
Sy Bam tit ISIE ek 
! godt 11246 mee 3 ; er 
Gompare thefe two Series with the two 
Series of the Theorem, and-you will find” 


is z -|- 


R= 


: Nea 
| eat, b=o, om Fidos = oa Ia 


32 x 


x rr n : | 
Bcc. got, b=0, 1 Gd =O I godt 
4 Yr 3 
m—o. &c. hence z will be =ay-4- cae 
: ‘ At eaig Td 


Re tr ny -\- bees pte: tiee | 
| 2 4 3das ? Ge ty.“ as 


to 


| MifceHanea Curiofa. 195 
to denote the whole preceding Term, which 
will be the fame Series as Mr. Newton has 
firft found. - Hie | 

By the fame Method, this general Pro- 
blem may be folv’d; the Abfciffe correfpond- 
ing to a certain Area in any Curve being gi- 
ven, to find the Abicifle, whofe correfpond- 
ing Area fhall be to the firft in a given Ra- © 
- to. . 
The Logarithmick Series might alfo be 
found without borrowing any other Idea, 
than that Logarithms are the Indices of 
Powers: Let the Number, whofe Logarithm 
we inguire, be 1-|-z, fuppofe its Log. to be 
az--ozz-|-cz3, &c. Let there be another 
“Number i-|-y; thereof its Logarithm will 
be, ay-|- byy-|-cy?, &e. Now if 1--z= 


1-/- yl, it follows, that az -|- bzz-|-¢z3, &c. 
ay -|-byy-|-cy?, &c. :: 2, 1. that is, az-—- 
zz --0z3, &c. = nay -|- nbyy -|- my? &c. 
Therefore we may find a Value of z-expreft 
by the Powers of y; again, fince 1-+<= 


a-ky' therefore z = 1 = aa 1, that is, 
Sa Sy. a ate Soa, iS 
ae bom IY I 2, 3 

y*®, &c. Therefore z is doubly expreft by 
the Powers of y. Compare thefe two Values 
‘together, and the Coefficients 4, 6, ¢, &c. 
will be determin’d, except the firft 2 which 
“may be taken at pleafure, and gives accord- 
ingly, all the different Species of Logarithms. . 


9:2. . An 


te RS ere ee ce: OPN 
MEE Ay Er 

- Te ‘ 

Must a 


196  ©Mifcellanea Curiofa. 


An Experiment of the Refraction 
of the Atr made at the Com- 
mand of the Royal Society, 
March 28.5699... 4 

By J. Lowthorp, 4, M. 


E took’ a~ Cylinder -of Caft-Brafs 
3 (Fiz. 33.) ABCD, and cut one end of 
it CD perpendicular ‘to the Axis ax, the 
other end AB enclin’d to it at an Angle of 
about 27°. 30. and therefore the Perpendi- 
cular to this enclining plain, pe, and the Axis 
of the Cylinder- ax comprehended an Angle 
pea of about 620. 30d. Thefe ends were 
groun’d very true upon.a Glafs-Grinder’s 
Brafs-Tool, and each of them ‘was compatft 
_about with a narrow Ferule of thin Brafs bb00. 
Into the upper fide of the Cylinder at EB was 
“folder’d the Brafs-Pipe EF} and into the un- 
der fide at 6 the other Brafs-Pipe GH; the 
former of thefe Pipes being about 3 Inches 
long, and the latter. 6 Inches. Upon the 
Plate ddd were fixt to two other Plates LL 
perpendicular to it and parallel to each other. 
Bach of thefe two Plates had an: Arch of a 
Circle € equal to the.Circumference of the 
Cylinder) cut out of its upper Edge, fo that 
when the Pipe GH was let :through ‘a-hole 
‘near. -the-middle of the: Plate ddd,:the Cy- 
linder fell into the Arches; and being fa- 


. ften’d there with Soder, the Axis ax laid pa- 


~kallel to the Plate.ddd and about an Inch ie 
| . sgt ie . ieee 2 ha 8 


UMifcellarea Cupafa. | 197° 


half above it. The perpendicular End of - 
“the Cylinder DC was clos’d with an Objeé 
Glafs of.a feventy fixth Foot Telefcope oo 3, 
and the. other end AB, with a vwell polith’d 
flat Glafs ff; which was carefully chofen to 
tranfit the Obj-& diftina enough notwith- 
ftanding its Obliquity to the Vifnal Rays. 
-The Ferules were well fild with Cement 
round about the Edges of the Glafs, and they 
Jaid flat and every where touch’d the fmooth 
Ends of the Cylinder, that they might firm- 
ly refift the preffure of the excluded Air. 
Inftead of a Ciftern (as in the Torricellian 
Experiment) we made ufe of the Inverted 
Siphon of Brafs (Fig. 34.) MNO, foder’d to 
the Plate gzg. One of the fides "MN ftood 
perpendicular to the Plate, and the other 
fide NO enclin’d to it, and was fupported. 
‘near the upper end O with a little prop &k. 
- Wethen placed the Cylinder (as in Fig.33.) 
upon a Table which was well faiten’ d to a 
firm Floor; the Pipe GH was let through a | 
hole, and the Axis laid almoft parallel to the 
fides of the Table, and the Plate ddd was 
nail’d. down to it. The Tube of the Tele- 
feope ff, with the Eye-glafs, was apply’d to 
the Object Glafs, and a Hair fix’d within 
it at the common Focus of both Glaffes in the. 
Axis of the Cylinder. continw’d, x. . Upon the 
Floor (under the Cylinder). we id the 
Plate ggg with the Inverted Siphon upon it, 
-and join’d M to H by the InfeSion of the 
Glafs Tube T. The Joints were very care- 
fully. clos’d with:Cement: And then they 
awere coyer’d over with pieces of a Bladder 
B - wee hard with ftrong Thread. ‘There 
; “QO 3 was 


ni qe aa iy Av. 
WT Oy pea eae a MaRS Ter Nee 
$ > 4 Sobel Sine igi eS 


198  MifceHanea Curwofa. 
was alfo a Bladder ty’d below each Joint at’ 
m, and when it was filld with Water it was 
tyd above it at 7; fo that no Air could 
come to the Cement, or infinuate it felf 
through its Pores or Siffures if any happen’d 
to be left unclos’d. pM 
It is not (1 think) an unneceflary trouble, 
that in this account of the Apparatus I have 
mention’d fo many minute Circumftances, 
for we found it difficult enough to exclude 
the Air, and almoft impoffible to difco- 
ver the very little holes through which fo 
fubtil a Fluid would freely enter and poflefs 
the Spaces deferted by the fubfiding Mer- 
-cury. But with all this Precaution the Ex- 
- periment fucceeded at laft, as 1 wifhd, af 
ter this manner. Ee ‘ : 
We plac’d the Obje& 2 (which was a black 
Thread fliding in a little Frame over a piece 
of white Paper) in the Axis of the Cylinder 
cx continu’d to it, we filled the Pipes and Cy- 
linder with Mercury; and having ftopt the up- 
permoft Pipe at F with the little lron-{topple 
K and clos’d it at the other Joints, welet the 
Mercury run out gently at O into the Blad- 
der v, till it remain’d fofpended at the ufual 
height (as in the Barometre) leaving the 
fpace above it between the Glafles 00 and ff 
void of Air. We then found the Object, 
which before appear’d in the Axis at x, raisd 
confiderably above it; and we reduc’d it to 
appear at x by removing it from @ to x. 
The Axis therefore, of the vifual Ray +a, 
(which was alfo the Axis of the Cylinder) «a, 
falling- perpendicularly on the void fpace in 
the Cylinder paft through it without any Re- 


— —— Mifcellanea Curifa. 199 
fra&tion: But emerging obliquely into the 
‘Air, it was refra@ted towards the Perpendi- 
cular pe, and there receiv’d a new Direction 
tox. And therefore the fpace ax fubftend- 
ed the Angle of Refraction acx; which we 
meafur’d and found as follows. . 
- The height of the Obje&t- Inches Depths 
above the Axis of ye 
 fual-Ray 2x the unre- ° 425 
‘ fracted bp ey 
The Diftance of the Ob- 
: je from the Refract- 6 
ing Plain, @c. about Ca 
oeepeeect Or 

Therefore the Angle of , i 
 -Refra@tion acx was — ¢ Cee Fae 

The Angle of Emerfion oy : 
_ pea (by the Conftrudti- 

on of the Cylinder) a” 
was oe 
Therefore the Angle of) 

Incidence pex== (=peap 62. 27- coe 

ate Od | | 
And therefore univerfally (according to 
the known Laws of RefraGtion) | 

The Sines of the Aiges & eesti 

of Incidence being — 3. 
The Sines of the paglc f bbs 
Emerfion are — — oe 

And the Refractive Pow-2 ss _-3 

er of the Denfe Air —-$ ; 

By the Refractive Power of a pellucid Bo- 
dy, limean that property in it whereby the 
Oblique Rays of Light are diverted from 
“their dire& Courfe ; and which is meafur’d 
Ne ‘ O 4 DY 


*. 


i? 


200. Mifcellanea Curiofa. ~~ 
by the proportional Differences always ob-— 
ferv’d between the Sines of the Angles of In-_ 
cidence and Emerfion. ngchs es. 

This Property is not always propor-— 


ie cb Nites aie tt 


me 
cor 


tional to. the Denfity (at leaf not to the 


Gravity) of the Refra@ing Medium. For 


the Refra@ive Power of Glafs to that” 


of Water, is as 55 to 34, whereas its Gra-_ 
vity, is as 87 to 34; that is, the Squares of 
their Refractive Powers are (very meat) as 
their refpective Gravities. And there are 
fome Fluids which though lighter than Wa-. 
ter yet have a greater power of Refraction ; 
thus the Refractive Power of Spirit of Wine 
(according to Dr. Hoek’s Experiments, AZ- 
crog. p. 220.) is to that of Water, as 36 to 
33, and its‘Gravity reciprocally, as 33.to 
36, or 362. But the Refra&ive Powers of 
Air and Water feem to obferve the fimple 
Proportion of their Gravities, dire@ly;.as I 
have compar’d them in. the following Table. 
The Numbers there exprefling the Refra- 
ction of Water are taken from the Mean. of 


-* Nine Obfervations at fo many feveral An- 


gles of Incidence, made Jar. 25. 1647. by 
Mr. Gafcoigue the ingeninos Firft Inventor of 
the Micrometer, and the ways of meafuring 
Angles by Telefcopes, and thofe of Air are 
produc’d by; the Experinient above related. 


* Iam indebted. for them to Mr. Flamfteet, who. had 


 cover'd them with his-Objervations, ‘andi feveral Paffages 
relating to them,. from.his, Letters to-Mr. Crabtree, which 


mere pappily prefery'd in the Time of our Civil War by. 


Me 


Sir Jonas Moor, ‘and Mr. Chriftopher Towneley ; and 


ere now in- the’ Hands ‘of Mt. Richard ‘Towneley of 


hg in Lancathire,: by-whow rhey were inparted to 
fie ay age oi ems 


Ts i ane: 
ts, 
gS peat 


Nine te 
eee Mite ye 
Daitat ad sete Me ete th Ay 


rr 


P i 


a 
f 
7 
: nis ' 
: 4 
F i ‘ 
j 
, w 
i ") 
Ni 
Hi 
‘ 
i 
, 
5 + 
igure 
Ph 
F 
“ri 4 et 3 
: 7 
D ° 


zag 
vy 
» 

Vass. 
I 
wi 


i 


; 


ERA We 
vals Bg 


| Mifcellanea Cuvofa. 201 

The (aflum’d) Sines of 1 Water. Air. _ 
the Angles of Inci- p150000: 100000 
dence through — J 

- The Sines of the corre-} | 
fpondent Angles of ?134400. 100036 
_Emerfion out of — J hae: 
eS pial ae $AA00 70. 85 36 
The Specifick Gravity) 

{Gf as 900 to 1 at the | : 
time of the Experi-.>34400.... § 38 © 
mént) of or (if as| gO: 
850 to 1) of —-——+-— J Y 


‘From hence it feems very probable that 
‘their Refpedive Denfities and Refractive 
Powers are in a juft Simple Proportion: And 
if this fhould be confirm’d by fucceeding Ex- 
periments, made at different Angles of Inci- 
dence, and with Cylinders continuing ex- 
haufted through feveral Changes of the Air, 
it would be more than probable that the Re- 
fraétive Powers of the Atmofphere are every 
-where, at all heights above the Earth, in pro- . 
portion to its Denfities and Expanfions. And- 
here it would be no difficult matter to trace - 
the Light through it, thereby to terminate 
the Shadow of the Barth; and (together with 
proper Expedients for meafuring the Quantity 
of Light illuminating an Opaque Body) to ex- 
amine at what diftances the Moon muft be 
from the Earth to fuffer Eclipfes of the ob- 
ferv’d Duration. . This Limitation is confide-. 

able enough in Aftronomy, abundantly to 
‘recompenfe the Trouble of profecuting fuch © 
anew Experiment. =. 

ee sao ae AA 


202 Mie tes Cores. | 


A Dim concerning a Mabal 
of Difcovering the true ‘Moment 
if the Sun’s Ingrefs into the Tro- 


pical Sines. : 
es E. Halley. 


T may perhaps pafs ee a Paradox, if bot 
feem extravagant, if I fhould affert that 

it is an eafier matter to be affur’d of the 
Moments of the Tropicks, or of the Times 
of the Sun’s Entrance into Cancer and Capri~ 
corn, than it is to-obferve the true Times 
of the Equinodtials or Ingrefs into Aries and 
Libra. know the Opinion both of Ancient 
and Modern Aftronomers to the contrary ; 
Ptolemy fays exprefly, Tas trav resrav tupaces 
~ Such venetrss ivan s And Ricciolus begins. his 
Chapter of the: Solftitial Obfervations with 
_thefe words, Mer:to Snellius, iz notis ad ob- 
fervationes Hafliacas, pronunciavit, Her culei effe 
laboris vitare in Solttitiis obfervandis errorem 
quadrantis diei, and this becaufe of the ex- 
ceeding flownefs of the change of the Sun’s 
Declination on the day of, the Tropick, be- 
ing not a quarter of a Minute in twenty 
four Hours. ‘This indeed would make it ve- 
sy difficult, nor would any Inftruments fuffice 
to do it, were the Moment of the Tropick 
_fo-be determin’d from one fingle Obferva- 
tion. But as three fubfequent Biediieone 
made 


Mifcellanea Curiofa. 202 

‘made near the Tropick, at proper Intervals 
of Time, I hereby defign to fhew a Method 
to find the Moment of the Tropicks capable 
- of all the ExaGnefs the moft Accurate can 
defire; and that without any confideration 
of the Parallax of the Sun, of the Refradi- 
ons of the Air, of the greateft Obliquity of 
the Ecliptick, or Latitude of the Place: All 
which are requir’d to afcertain the Times of 
the Equino¢ctials from Obfervation, and 
which being faultily aflum’d, have occafion’d 
an Error of near three Hours in the Times 
of the Equinoétials deduced from the Tables 
of the Noble Tycho Brahe and Kepler, the 
Vernal being fo much later, and the Au- 
tumnial fo much earlier than by the Calculus 
of thofe Famous Authors. es 

| Now before we proceed, it will be necef- 
fary to premife the folowing Lemmata, fer- 
ving to demonftrate this Method, wz. 

1. That the Motion of the Sun in the 
Ecliptick, about the Time of the Tropicks, 
is fo nearly equable, that the difference 
from Equality is not fenfible, from five days 
before the Tropick, to five days after: And 
the difference arifing from the little Inequa- 
lity that there is, never amounts to above 
3 of a fingle Second in the Declination, and 
this by reafon of the nearnefs of the Apo- 
gaon of the Sun to the Tropick of Cancer. | 

2. That for five Degrees before and after 
the Tropicks, the differences whereby the Sun 
falls fhort of the Tropicks, are as the verfed 
Sines of the Sun’s diftance in Longitude from 
_ the Tropicks, which verfed Sines in Arches 
under five Degrees, are beyond the utmoft 
as a vie nicety 


I 


204 7." feline Char itd 


nicety of Senfe, as the Squares of thofe Arches. 


From thefe two follow a third: 


3. That for five'days before ant afést the 
Tropicks, the Declination of the Sun falls 
fhort of the utmoft Tropical Declination, by 
Spaces which are in duplicate Proportion, 


or as the Squares of the Times by which — 


the Sun is wanting of or paft. the) Moment 
of the Tropick. | 
Hence it is evident that if éhe Shadows 


of the Sun, either in the Meridian or any 
other Azimuth, be carefully obferv’d about 


the Time of the Tr opicks, the Spaces where- 


ae 
ee 


by the Tropical fhade falls fhort of, or'ex= __ 


ceeds thofe at other Times, are always. pro- 


portionable to the Squares of the Intervals 


of Time between thade Obfervations and the ~ 


true Time of the Tropick, and ‘confequently 
if the Line, on which the Limits of the fhade 


is taken, be made the Axis, and the corre- 


fpondent Times from the Tropick expound- 
ed by Lines, be erected on their refpedtive 


Points in the Axis as Ordinates, the Extre-_ 


mities of thofe Lines fhall touch’ the Curve 


of a Parabola; as may-be feen in the Fi- 


gure: Where a, b,c, e, being fuppofed 
‘Points obferved, the ‘Lines. aB, bC, cA, 
ed, are refpedively: proportional ‘tO. the | 
Times of each Obfervation before or after 


the Tropical Moment in Cancer. 


| This premifed,. we fhall be able to han t 


the Problem:of finding the trne Time of the 


Tropick by ‘three Obfervations, to this Geo- 


“ metrical ones having three: Points in a Paz 


rabola A, B,C, or Ay F,C given, together 


ane the direftion of the Axis, to find the 
si 


—  Mafcelanea Curtofa. 208 
Diftsngeor thofe Points from the Axis. Of 
this there are two Cafes, the one when the 
- Time of the fecond. Obfervation B is pre- 
_ cifely in the middie Time between A and C: 

‘In this Café putting t for the whole Time 


. between A and C, we fhall have Ac the In- 


terval of the remoteft Obfervation A from 
the Tropick by the following: Analogy, 

/ AS-2ace—bce to 2acei bc::! So ist t 
or AE:to Ac the Time of the remoteft 
_ Obfervation A from the Tropick. 

But the other Cafe when the middle Ob- 
fervation is not exadly in the middle, be- 
tween the other two Times, as at F, is fome- 
‘thing more -operofe, and the whole Time 


from A to C: being: put =t, and from A to 


& F =, €@-=c,-and b oe be the Theorem 
| Bs ttc—bss 


will ftand thus - ma Act the Time 
2tC—2 Ws Ss. 
- fought. 

To illuftrate this Method of Calculation it 
may perhans be. requifite to give an Exam- 
_ ple or two for the fake of thofe Aftrono- 
mers that are lefs inftru@ted in the Geome- 
‘trical part of their Art. 

Anno 1500, Bernard Walther, in the Month 
of Fune, at Nuremburg, obferv’d. the Chord 
of the diftance. of the Sun from the Zenith 
- bya large Parailattick Inftrument of hie 

as follows : 


Sune 2. “43461: Gunes Se: 44975: 
. Fune 9. 44934. and. Fune 12. 44883. 


: June 16. 44990 ‘Funei6. 44990. 


In 


ee Mifitlanes Curiofas 


In both which Cafes the middle Time is 
exactly in the middle between the Extreams, 
and therefore in the former three, a c=§33, 
bc=477 and t, the Time between being 14 . 
days, by the fir ft Rule, the Time of the. 
Tropick will be found by this Proportion, as 
_§89 to 8273:: So; t or 7 days to 9 days 
2oh. 4’. whence the “Tropick, Anno 1500. -is 
concluded to have fallen Fune and. 20h. 2’, 
Inthe latter. three, ac is ==) 1e7 7, and 
bc=15, and the whole Interval of Time 
is 8 days = to t; whence as i99 : to 2067 
‘: fo is 4 days to. 4d: 3he 37. which taken 
: from the 16th day at Noon, leaves 1144+ 20h. 
23. for the Time of the Tropick, agreeing 
preliaas the former to the third part of an 

our 


_ Again, Anno 1636. Gaffendus at Marfeilles, 


obferv’d the Summer Solftice by a Gzomon of 


55 Foot high, in order to determine the Pro- — 


portion of the Gnomon to the Solftitial fhade, 
and he hath lett us thefe Obfervations, which 
may ferve as an seu for the fecond 
Rule. : 


'Fune 19. St. N. fhadow 319766 parts, whereof 
the Guomon was 89428. 


“June 20. 31753 
Sune-21. 2 1RkeE 
Fume 22.0 208s 31759 


Thefe being divided into two Sets of three 
Obfervations: each, viz. the roth. 20th. and 
22th. and the 1 oth. 21th. and 22th. we fhall 
have in the firft three c= 13 and oO 7. 
t= 3 days, sco i and i in the fecond c = : 
, ; ~~ BD 


Mifcellanea Curiwfa. 207 
and b= 7, t= 3 and s=—,2.” Whence, ac- 
cording to the Rule, the roth day at Noon 
the Sun wanted of the Tropick a Time pro- 
portionate to one day, as ttc--ssb to 
$40-+2b55, that is, aS 110 to'64 in the 
firft Set, or 107 to 62.4in the fecond Set ; 
that is, 14-17-15’. in the firft, or 14- 174-295’. 
in the fecond Set: So that we may conclude the 
Moment of the Tropick to have been ‘Sune 
rod. 47h. 207. in the Meridian of Marfelles. 

Now that thefe two Tropical Times thus 

obtain’d, will be found to confirm each o- 
thers Exactnefs from their near Agreement, 

“appears by the Interval of Time between 
them; vz. 14- 2h. 30. lefs than 136 Julian 
Years: whereof 14. 1h. Q’. arifes from the de- 
fect of the length of the Tropical Year from 
the Julian, and the reft from the Progreffion 
of the Sun’s Apogaon in that Time; fo that 
no two Obfervations made by the fame Ob- 
ferver in the fame Place, can better anfwer 
each other, and that without any the leaft 
Artifice or Force in the management of 
them. 

What were the Methods ufed by the An- 
_cients to conclude the hour of the Tropicks, 
Ptolemy has no where delivered ; but it were 

to have been wifhed that they had been a- 
ware of this, that fo we might have been 
more certain of the Moments of the Tro- 
“picks we have receiv’d from them, which 
would have been of fingular ufe to deter- 
mine the Queftion, Whether the Sun’s Apo- 
geon be fixt in the Starry Heaven, or if it — 
move, What is the true Motion thereof? 
It is certain, that if we take the Account 

} : of 


208 Maifcellanea Curiofa.. 
of Ptolemy, the Tropick faid to be obferw’d 
by Euttemon and Meton, Funii 27. mane, An- 
#0 432. ante Chriffum, can no ways be re- 
concil’d without fuppofing the Obfervation 
made the next day, or Fune 28th in the 
Morning. And Prolemy’s own Tropick ob- 
ferv’'d in the third Year of Antoninus, Anno 
Chrifft 140. was rahe ssi on the 23th and 
not the 24th day of Yune, as will appear 
to thofe that fhall duly confider and com- 
pare them with the length of the Year de- 
duced from the diligent and concordant Ob- 
fervations of thofe two great Aftronomical 
Genii, Hipparchus and Albatam; eftablifh’d 
and confirm’d by the Concurrence of all the 
Modern Acctracy. For thefe Obfervations 
give the length of the Tropical Year, fuch | 
as to anticipate the Fulian Account only one 
day “in 300 Years; but we are now fecure 
that the faid Period of the Sun’s Revolu- 
tion docs anticipate very nearly three days 
in 400 Years; fo that the Tables of Ptolemy _ 
founded on that Suppofition, do err about a — 
whole day in the Sun’s Place, for’ every 240) 
Years. Which principal Error in fo Funda-— 
mental a Point, does vitiate the whole Su- | 
perftructure of the Almageft, and ferves to 
convict its Author of want of Diligence, or 
Fidelity, or both. 

But to return to our Method, the great’ 
Advantage we: have. hereby,” is, that any” 
very high Building ferves for an Inftrument, 
or the Top of any high Tower or Steeple, 
or even any high Wall whatfoever, that may. 
be fufficient to intercept the Sun, and caft a 
true eotea Nor is the Pofi tion of the Plane. 

OR 


Mifcellanea Carole. : 209 


bn which you take the fhade, or that of the 
Line therein, on which you meafure the Re- 
-cefs of the Sun from the Tropick, very ma- 
pterial; but) in’ what wey foever you: difeove er 
“it, the faid Recéfs will be always in the fame 
- Propor tion, ‘by reafon of the fimalnefs of the 
Angle, which is not fix Minutes in the firft 
five days: Nor need you enquire the height 
-or diftance of your Buildings, provided it be 
ivery great, fo as to make the Spaces you | 
-meafure large and fair. But it is convenient 
*that the Plane on which you take the fhade_ 
“be not far from Perpendicular to the Sun, at 
‘Teaft not very Oblique, and that the Wall 
which cafts the fhade, be ftraight and fmooth 
‘at Top, and its Direétion nearly Haft and | 
Welt, for Reafons that will be well under- . 
ftood by a Reader skilful in the DoGrine of 
‘the Sphere. And it will be requifite to take 
‘the Extream greateft or leaft Deviation of 
‘the fhadow of the Wall, becaufe the- fhade 
“continues for a good Time at a ftand, with- 
“out alteration, which will give the Obferver 
eifure to be aflar’d of what he does, and not 
be furpriz’d by the quick tranfient Motion 
ef the fhade of-a fingle Point at fuch a dl- 
tance. The pr incipal Objection i is, that the 
Penumbra or Partite fhade of the Sun, is in 
‘Its Extreams very difficult to diftinguihh from 
‘the true fhade, which will render this Obfer- 
vation hard to determine nicely. But if the 
‘Sun be tranfmitted through a Telefcope, after 
the manner us’d to take his Species in a Solar 
‘Eclipfe, and the upper half of the Object- - 
‘giafs be cut off by a Paper palted thereon, — 
and the exact upper Limb of the Sua be sue 
Pp - jul 


by ae i, hE tie Re SS) cep 


210 Mifcellanea Curtofa. 
jut Emerging out of, or rather continging 
the Species of the Wall, (the Pofition of the 
Telefcope being regulated by a fine Hair ex- 
tended in the Focus of the Eye-glafs) | am 
affur’d that the Limit of the fhade may be 
obtain’d to the utmoft Exaétnefs: And of 
this I defign to give a Specimen by an Obfer- 
vation to be made in fume next, by the help 
of the high Wall of St. Paul’s Church, Lon- 
don, of which fome following Tranfaction 
may give an Account. In the mean time 
what I have premis’d may fuffice to fet others 
at work, where fuch or higher Buildings are 
to be met with. I fhall only Advertife, that 
the Winter-Tropick: by this Method may be 
more certainly obtain’d than the Summer’s, 
by reafon that the fame Gwomon does aftord 
-a much larger Radius for this manner of 
-Obiervation- 


: Mifeellanea Curipfa. Oe i ae 


A Scale of the Degrees of 


ss ae Oe 


T be Siens and ‘Defcraptions of the 
pete Deorees of Heat. 


HE Warmth of the Winter 

4ir when Water begins to 
freeze. This.is known accurately 
by placing a Thermometer in Snow 
prefs'd clofe together at the Time 
_jof a Thaw. 

The Warmths of the Winter Air. 

The Warmths of the Air in 
Spring and Autumn. 

The Heat of the Air in Summer. 

The Heat of the Air at Nooz in 
the Month of July. 

The greateft Heat that a Ther- 
mometer acquires, by the contact 
of a Humane Body ; which is much 
the fame with that of a Bird brood- 
28 upon its Eggs. 

The nearly greateft Heat of a 
\Barh, that a Perfon holding his 
Hand fteady and immoveable in the © 
fame, can endure for fome time. 

17412-/ The greateft Heat of a Bath, 
that a Perfon holding his Hand 
| ffteady and immoveable in the 
me) P a fame, 


412  psteetanen Coriohae 


ae can endure for fome time. q 
| 2° Ori The Heat of a Bath by which J 
i melted Wax fwimmipg upon it, 7 
| a begins to grow ftiff, and lofe its” q | 

a Tranfparency. | 4 
L243] Oa ie Ted: Dra Bath by which 

| |Wax fwimming-upon it, is. melted § 

land preferv’d in a State of Fluidi- ' | 

ty, without Ebullution. 4 
The middle Degree of Heat, beat . 
tween that by which Wax is melt-- : 
led, and that which makes Water | 4 
, boll, i , 
The Heat . by wien Water is S| 
gs to boil vehemently; and a 
Mixture of 2 parts of Lead, 3 off) 
Tin, and 5 of Bofmuth, cooling, f 
begins to harden. f 

Water begins to boil witha Heat! 7 
of 33 parts, and by boiling, hard= 
ly conceives a ‘greater Heat than | 
that of 34. parts. 

Bat Iron. growing cool, when if 
Ihas a Heat of 35 OF "36 parts, ceafes| 
to make any Ebullition when warm q 
Water falls drop by drop upon it; 
as it.does alfo with a Heat of 37 
parts, when cold Water falls on it 
| in the like manner. . : | 
4005 “Io3.) The leaft Heat, by. hich a Mixs | 

‘ture of 1 part of Lead, 4 Of Tiny | 

land 5 of Bifmuth is liquefied and | | 

| _{preferv’d in a State of Fluidity. 

48. 3-|. The leaft Heat, bywhich 4Mist | 

| ture of equal parts of Tis and Bif4 “| 
uth is, aN BRE- This Mixtur@ 

gr0 io | 


ae 


a“ | 


ee Guta” erg” 


growig cool, when it has a Heat 
of 47 parts, is coagulated. 
ie bs meahe Heat, by Which a Mixture 
fot 2, parts of Tin and t of Bifinuth 
is liquefied ; as alfo of 3 parts of 
Tin and 2 of Lead. But a Mixture 
of 5 parts of Tiz and 2 of Béfwuth 
(cooling) dees with this Degree of 
| {Heat become hard: And the fame 
| Icome to pafs in a Mixture of e- 
Jes qual parts of Lead and Bifmuth. | 
32 “The leaft Heat by w hich a Mix- 
Iture of 1 part of Bifmuth and 8 of 
ia (Tin is liquefied. Tin by it felt ts 
fus’diwith a Heat of 72 parts, and 
|. growing cold, hardens with a Heat. 
of 70 parts. | 
Ae 34+ The Heat by witch Bifmuth i$ 
ffus’d; as alfo a Mixture of 4 parts 
of Lead and 1 of Tin. | But a Mix- 
ture of 5 patts of Lead and 1 of 
' \Ti when fas'd, and growing cold, 
ee hardens with this Degree of Feat. 
41 -The ‘leaft Heat by which Lead 
is melted. Lead melts with a Heat 
of 96 or 97 parts,.and growing 
(cold, hardens with a. Heat of 95 
eh ers 
“114.444 ‘The Heat with’ which Fery Be 
hee (growing cool) wholly ceafe 
fhinins in-the Night; as alfo, that 
-{Fleat: With which (crowing ‘warm ) | 
“tthey- firft begin to fhine in the 
the Darknefs of the Night, bue 
with a faint and Fora Lieht, 
fach as can fearce be difcern’d. 
Posy’ This 


96. 


Ay Se 


Ree ret AeA HET SHEER Se Te aD LIOA RES a ean 


uf [This Heat liguefies a Mixture of 4 


136-\43- 


192.| 5: 


equal parts of Tim and Regulus Mar- 
‘is; and a Mixture of 7 parts of 
Bijmuth and 4 of the fame Regulus 
(growing cool) hardens with the 
fame Degree of Heat. 

The Heat by which Fiery Bodies 
do in the dark Night appear bright 
and fhining, but not in the Twi- 
light. A Mixture of 2 parts of 
Regulus Martis and 1 of Bifmuth, 
as alfo of 5 parts of Regulus Afar- 
tis and 1 of Tin, growing cool, 
will at this Degree of Heat be- 
come hard. The Kegulus by it felt, 
hardens with a Heat of 146 parts. 

~The Heat by which Fiery Bodies, 
in the Twilight, a little before the | 
Sun’s rifing or after his fetting, do 
fhine difcernably.; but not at all - 
in the clear Day-light, or at leaft — 
very obficurely. han oie 

The Heat of a fmall Culinary — 
Fire made of Sea-Coal, © burning 
freely by it felf without the help 
Bellows. The fame is the. Heat 
of Iron, as Red-hot as it can be 
made in fuch a Fire. The Heat of © 
a fmall Culinary Fire made of | 
Wood, is fome little matter grea- 
ter, viz. about 200 Or 210 parts. © 


1And the Heat of a large Fire is” 


{till greater, efpecially if it be blown - 
up by the Bellows. : 


Ja 


~ Mifcellanea Curiofa. 215 
- In the firft Column of this Table are the — 
feveral Degrees of Heat, going on in at 
-Arithmetical Progreffion, beginning with 
that Degree of Heat, which there is in the 
Air in Frofty Weather, when Water makes 
the firff Advances towards Freezing , beginning 
the Account from this, as the loweft Degree 
of Heat, or common Terminus of Heat and . 
Cold) and fuppofing the external Heat of 
a Humane Body to be rated at 12 parts. In 
the fecond Column are.the Degrees of Heat 
in a Geometrical Proportion, fo that the 
fecond Degree is double the firft, the third 
double the fecond, and fo on; the firft De- 
gree being that external Heat of a Humane. 
Body, proportion’d to the Senfe. But now 
*tis manifeft from this Table that the Heat. 
of Boiling Water is almoft 3 times greater 
than that of a Humane Body; and that the 
‘Heat of melted Tiz is 6 times, of melted 
Lead 8 times, of melted Regulus 12 times, 
and of ordinary Culinary Fire 16 or 17 times 
greater than the foremention’d Heat of a 
Humane Body. : 3 

_ This Table was made by the help of a. 

Thermometer and Red-hot Iron. By the. ~ 
Thermometer I found the Meafure of all 
the Degrees of Heat as far as that by which. 
Tin is melted; and by the hot Iron I found. 
the Meafure of the reft. For the. Heat 
which hot Iron does communicate to. cold 
Bodies contiguous to it in a given time,: 
(that is the Heat which the Iron it felf 
fofes) is as the whole Heat of the Iron. And 
therefore if the Times of Refrigeration are. 
ORE ie RP 4 ) taker 


Ry SL ee COE a ee 
Sit 


do en ah AR ae RNa eS SA a Lad 


216 Mifeel anea Curt i acme, | 


taken aqinils the Deoress of Heat fhall be? 
ina Geometrical Propor tion, and ote ena | } 
ly may cafily be found by a Table of Loga-— 


rithms. © Firft of all: therefore I found by a_ 
Thermometer made of Linfeed Oil, ‘that if 
when the laftrument' was “placed in melting 
Snow, the Oil occupied’ a Space of 19000" 
parts, the fame Oil rarified by a Heat of the 
frft Deptee (that is by that of a’ Humane’ 
Body) would extend to 16256 parts; and 
by the Heat of Water beginning to boil, to. 
¥o70§° parts; -and by the Heat of ‘Water 
boiling veheinently, £0. 10725 parts’; and: by 
the Heat pe melted Tin (cooling, ‘and be-) 
ginning to be of the Confiltence of an Amal- 
ama) ‘to 11516 parts ; and by the Heat of 
the fame Tin when "tis quite barden’d, to 
11496 parts.’ Therefore the Oil.was rarified 
in the proportion of 40°to°39, by. the Heat. 
of a Flumane Body$ and in the: proportion: 
of 15 to 14, by the Heat of boiling Water 5° 
and in the proportion of 15 to 13 , by the’ 
Feat of the melted Tin, be: sinning: to come. 
to the Confifteace of an Amalgamias and in 
the proportion, of 23 to\26; “by. rth “Heat of, 
the fame Tin quite hardned." ay ay 
AAT Be rechten of Ait with An wn Bet | 
gree‘of Heat, was 10 tives greater than that? 
of Oil; , and th é Rarefa@ion of Oil nearly” 15, 
times greater ‘than that of Spirit’ ‘of ‘Wine ‘i 
Now’ th hefe ‘thittes thus found. fa ppofing cn 
Degrees’ of Heat'in’ the Oir 4 THe rope 
tional’to ‘its’ Rarefattion, and che’ é of 4) 
Humane’ Body to’ be 12° ber, froin hence 
the Heat Of: Water wheat ; begitis ‘to boil, iy 
i A comes 


4 
a 


- Mifcellanea ue oi 2.1 7 


“comes to be 33 parts, and when it boils: ve- 


nemently, 34 parts; and the Heat of melt- 


ed Tin beginning to come to the Confiftence 


of an Amalgama, 72 parts; -and the Heat 
of the fame, when in cooling "tis: come to — 
downright Hardnefs, 70 parts. And having 
determin’d thefe Things, in order to find 
out the reft, I heated a piece of Iron ’till it 


~ was Red- hot enough, and taking it out of 


the Fire with a pair of Tongs that were 
alfo Red-hot, and I it in a cool place, 
where the Wind blew conftantly. Then 
putting oe it little pieces of Metals and 
various other liquable Bodies, I obferv’d the 


times of Refrigeration, "till all thofe melted 


€ 


parts having quite loft their Fluidity, be- 
came hal’d and folid- again, and the Heat of 
the Iron was equal to that ‘of a Humane Bo- 
dy. . Then fuppofing the Exceffes, of the 
Heats of the Iron and the liquefied Parti- 
cles approaching to Induration, above the 
Heat of the Atmofphere founded by the 
Thermometer, to be in a Geometrick Pro- 
ereffion, when the Times are in an Arith- 
metick one; by this means all the Degrees 
of Heat were. difcover’d. But ’tis to be ob- 
ferv’d that I plac’d the Iron not in a ferene | 
and quiet Air, bat in a Wind blowing uni- 
formly, fo that the Air which was heated by 
the Iron might always be carried away by 
the Wind, and a cold Air with an uniform 
Motion might Hicceed. in the place of. “it. 
For thus, equal parts of the Air were heat- 


‘ed in equal times, and acquired a Heat 


pene to that of the Iron. But the 
\ Degrees 


Ee TS ON ORE ROT Ta LEE ue Sob EU EPG ERO ENC Ce sees the eye ay aes 


918 Micellanea Curtofa. es 


Degrees of Heat found by this Method had 
the fame Proportion among themfelves, that 
thofe had which were found by the Ther- 
mometer; and therefore the Aflumption, 
that the Rarefactions of the Oil were pro- 
portional to the Degrees of Heat, was a 
juft and true one. ; * 


™~ 
i 
The 4 
id 
i} 
i 
/ 
s 
° 


cal cael “hig | i ~ , 
— — Maifcellanea Curiofa. 219 


The Properties of the Cate- 

| aria. 
_ By David Gregory, M.D. Savi- 
Profeffor of Aftronomy, and 

Fe « Gee aD | 


PROP.L PROBLEM. 


To find the Relation of the Fluxion of 
the Axis, to the Fluxion of the Ordz- 
dinate im the Catenaria, 


ET FAD be a Catena hanging on the 
|_j Extremites F and D, the loweft point 
of which (or the Vertex of the Curve) is A, 
the Axis AD perpendicular to the Horizon, 
and the Ordinate BD parallel to the fame. 
We are to find the Relation between Bb or 
De’, and df; fuppofing the point 6 infinitely 
near to B, and bd parallel to BD, as alfo 
DS to BA. 
From the Principles of Adechanicks, ’tis 
plain that three Powers which are in Equil:- 
brio. are in proportion to one another, as 
three right Lines parallel to their refpective 
Directions (or inclin’d in any given Angle 
to them) and terminated at their mutual In- 
terfection. 
vu And 


_. perpendicularly upon Dd, and by which it 


— 220 Maifcelanea Curiofa, ees 
And confequently if Dd expounds the ab- — 
folute Gravity of the Particle Dd (as it will 
be in a Catena equally thick) then dS will re- 
prefent that part of the. Gravity which ats 


comes to pafs that dD. (being by the flexibi- 
lity of the Chain moveable about d) endeavours 
to bring it felf into.a Vertical Pofition. And — 
therefore if Sd (Cor-the Fluxion of the Ordi- 
nate BD) be Gonftant, the AGion of the Gra- 
vity exerted perpendicularly upon. the cor- 
refpondent parts of the Cztexa Dd, will alfo 
be conftant, or every where the fame. Let 
this Action or Force be expounded by a. 
Farther ; From the above cited Propofition 
_in Mechanicks, Dds or the Fluxion of the 


aE REN GR re Cle peat arg Sg I aa 


Axis AB, will expound the Force to be ex-- 7 
erted in the direction dD, which is. equiva- — 
lent to the former Exdeavour of Dd (by which © 


it tends to bring it felf into a Vertical Pofiti- 
on) and 1s fufficient to hinder it. 

But this force arifes from: the Linea Gra- 
vis DA pulling with the direction. dD,, and. 
is confequently (all the reft continuing as be-. 
fore) proportional to that Line DA. ‘There-. 
fore dd, the Fluxion of the Ordinate, js to 
$D,. the Fluxion‘of the Abfeciffe, as the con- » 


SSSA areca sah. 


Itant right Line 4 to the Curve DA. Q: @ 


, 7 . 2 a 4 : 
, . a EN ‘ iggs ‘ A ore pa Pee! i 
4 ; . ee. oP e's ae | ate 4 
C; 0. B..Qrobaae ae oe ee 
rs ° ; : 2 : ; of states 


‘IE the right Line DT touches the Catena- t 
ria, and meets the Axis AB produc’d in T, © 
then will DB: BI: (2c 2Deag a.DA,& 


Curve. pee 
ie PROP. 


Bee: Mifcelanea Curiofa. ore 


| ee F: I. THEOREM. 
: (Fig.34.) If upon the Perpendicular AB. 


as an Axis, and the Vertex A, an E- 
qailateral Hyperbola AM be defcribd, ° 
whofe Semiaxis ACS a; as allo upon 
the fame Axis and Vertex, a Parabola 
“AP whofe. Parameter is quadruple the 
Axis of the Hyperbola, and the Ordt- 
pate of the Hyperbola HB be always 
prodac’d till WE be equal to the Curve 
"AP: I fay then, that (making BD ana 
BF, equal) the Curve FAD, ia which 
the Points F, D, are pofited, is the Ca- 
~ tenaria. 


Put AB— +; then Bbh=-~, and BH = 


N/ sax-l-xx ; ‘whence (from the Method of — 
Fluxions) the Fluxion of BH, that is mb = 
ax-| sexe | | | 
Again, fince the Parabola AP 
ec. 

‘has for its Parameter 82, BP fhall = i 8ax; 
Whence-the Fluxion of BP, that is p= 


- BAN 
1, Wherefore the Fluxion of the Curve 
af DAR | | 

| AP 


rads Me hi SL Aim 


222 Mafcellanea Curiofa. — 


AP ( = ae V wpt-| Pn’ ) — f= aa? 


| | dana 
NV oak? line: ; which is ot to 


xt ioe 
as appears by multiplying both Numerator 


Cena 


and Denominator into yh aie Das And fince 
LE is every where = == AP thie Fluxion of 


9. 


Ia : 
HF that is me sf, fhall = ————-. But 
ee 
axfxe 


we have hitherto found mb = 


| (aos 
Therefore sf (the Fluxion of BE the Ordi- . 


3 AX 
nate Le the Coenanan — 


3 and 


ty aa 2ax-|-K 
confequently the Fluxion of the Curve AF | 


ene 


fda is, Ff= V sf Let Ve x +3? ) 


Ax=\- 20d 


PS x 


is = +——. 


Ve le 


™ the Plowing Quantity of 


which 


Mifcellanea Curtofa. 223 
° ai | : ; en are 
which was fhewn but now to be V azole 


And therefore AF = Nate. And ’tis 
plain, that the Fluxion of the Ordinate BF, 


AX ° 
or ———-——,, is to x the Fluxion of the 
: V 2ax-lox , | 


Abfciffe AB, as the conftant Quantity 2, to 
the Curve AF; which was the Property of 
the Cuatenaria found above. Therefore the 
points of the Catenaria are rightly determin’d - 
by the foregoing Conftruction. Q: E: D. 


won OL. 1 


It is manifeft from the Conftru@tion, that 
BF the Ordinate in the Catezaria, is equal to 
the Parabolick Curve AP, taking away BH, 
the correfpondent Ordinate, of the conter- 
‘minal Hyperbola AH. 


GO ROL. IE. 


’*Tis~plain from the Demonftration, that 
the Curve of the Curenaria AF, is equal to 
BH the correfpondent Ordinate of the con- 
terminat Equilateral Hyperbola. For fince 
the Fluxions of thefe Lines are equal, and the 
Lines themfelves do arife together, it is ma- 
 nifeft that they are always, and every where 
equal. Whence, giving the Catena, AC or a 

will be given alfo,.as being equal to the Se- 
| maxis 


224 Mifcellanea Curwofa, 


miaxis of the Equilateral Hyperbola, whofe - 
Vertex is A, and whofe Ordinate belonging — 


the Abfciffe AB, isequal to the Catena AD. 
COROL: 1. a 


‘Ail the Catenaria are fimilar to one ano- 
ther; as being generated from the fimilar 


5. 


a 


ConftruGion of Similar, and firnilarly pofited 


Figures... From whence it follows, that two 


right Lines fimilarly inclin’d to the Horizon, 


carriéd thro’ the Vertices of the Catenaria, will 


eut off fimilar Figures, and proportional to the | 


Lines cutting off the Portions of the Cate- 
| NATIA. ; 


CoRG EL” ae 


If the Catena QAD be fulpended on the 


points Q and D, which are unequally high, 
the part FAD of the Curve remains the fame 
as if it.were fufpended by the points F and 
D, which are equally high. Fort it is no 
matter, whether the point be fix’d to- the 
Vertical Plane or not: rat 


ratolet eee ioe 


| Ny Soe, Fhed 

If the force of the Cutesa drawing in the 
Dire@tton dD, be divided (as is commonly 
known) into. the force as d/ acting with an 
Horizontal DireGion, and the force as SD 
witha perpendicular Direétion : ‘Then it fol+ 

lows, that the forceo(in the end of the Ca- 


\ ! tena) . 


PX 


Bia en eg Mee ole Sy 


A 


: Mifcellanea Curiofa. 225 
tena) of approaching dire@ly to the Axis, is — 
‘to the force of defcending perpendicularly 
in the fame (or that part of the fuftaining 
force that acts in the direction BD, is to that 
“part that acts in the dire@tion DJ) as the 
Semiaxis of the Conterminal Hyperbola AH, 
to DA the length of the Catena to the Ver- 
‘tex. Whence, the Catena being daveb: this 
Ratio is alfo given. And in the fame Ca- 
tena, fafpended with different degrees of 
Laxity, that Horizontal force, is as the Axis 
‘of the Conterminal Hyperbola; fince DA 
‘remains the fame, if, the Extremities be 
equally high. : | 


CORO: VL 


_. The Catena placed in an Inverted Pofition 
in a Vertical Plane, maintains its Figure and 
does not fall down; and fo makes a fine 
“Arch or Formx. That is, very fmall hard 
flippery Spheres, difpos’d in the Inverted 
Catenaria, will form an Arch, no part of — 
which will be thruft inwards or outwards by 
the reft, but (the loweft Points continuing un- 
‘movd) it is preferv’d by vertue of its Fi- 
‘gure. For fince the Pofition of the Points 
of the Catenaria, atid the Inclination of the 
“parts to the Horizon, is the fame, whether 
it be in the Pofition FAD, or in an Invert- 
ed Pofition, provided the Curve be ina Plane 
that is perpendicular to the Horizon, it is 
evident that jt preferves its Figure unchang- | 
ed, equally in one Pofition as the other. 
“And on the other hand, the Cztenaria are 

the 


Pe Te GS nce eR) 


226 Mifcelanea Curiofa. a 
~ the only Genuine Arches or Fornixes. And 

an Arch of any other Figure, is for this 
-reafon only, fuftain’d, becaufe a Catenarta. is” 
included in the thicknefs of it. For if it 
were very thin, and confifted of parts that 
were flippery, it would not be fuftain’d. 
From the foregoing fifth Corol. it may be ga- 
ther’d with what force an Arch thrufts the 
Walls outwards, that it ftands upon; for 
this is the very fame with that part of the 
force Cfuftaining the Catena) which draws 
with the Horizontal direGion. All other 
Matters requir’d in the ftrength and firm= 
nefs of Walls, that have Arches fet upon 
them, are Geometrically determin’d from 
this Theory; which are the principal Things 
in Building. ee | | 


COROL | vit 


If inftead of Gravity, any other force were 
fuppos'd acting in like manner upon a flexi- 
ble Line, the fame Curve would be produced. 
Ex. gr. Suppofe a Wind blowing: equably, 
and in directions parallel to a given right 
Line, the Line thus inflated by the Wind, 
would be the fame with the Catenaria. For 
-fince all things that were confider’d in Gra- 
vity, obtain in this other force, ’tis plain 
that the fame Curve will be produced. 


PROP 


mM ifcelaned Curis fe. a7 


PROP. Ill. THEOREM 


(Fig. 35.) The Hyperbola AH continuing 
- 45 before, if through A be drawn the 
- right Line GAL perpendicular to the 
Axis AB, and the Curve KR be de- 
feria of fuch a Nature, that BK be 
_ 4 third proportional to BH and AC, 
and to the right Line AC be applied the 
Reétangle AV equal to the Interminate 
Space ABKRLA; then fhall the Point 
F (the Concourfe of the right Lines 
HB, VG) be iz the Catenaria. | 


2 


; : a 
For by Conftru@ion BK = —; 
2 . V xan x? 
wherefore the Fluxion of the Space 
ee ih pe : ; 
ABKRLA (=BKkb=BKx Bb) = ——----——. 


pane 
Space ABKRLA 


And fince BF = ——-— , and AC 


C 
is given, the Fluxion of BF fhall = 
' the Fluxion of the Space ABKRLA 


RATT 


AC 
Q2, ae 


EE SEER ; eer 


Se oe 


228  Mifcellanea Curiofa. 


re But in the Conftruétion et the” 


V 2ax-tx 2 


foregonig ea tion, a cee of the Or 


Axe 


ee ax | i Roi 4 
dinate BF, was = ———, ‘Therefore. 


Wl dash Oe 


this Conftrudion amounts to the fame with | 


Catenarias PG ame apeee 1 f 
‘conoe 


As in the foregoing Propofi tion, the Catena: i 
ria is defcrib’d from the length of the Para- 
bolical Curve given; fo in this, the defcrip- 
tion of it depends upon the Quadrature \f 
the PURSE in vee x7y” <= a* ome 2axy”. i | 


: : ; ; ~ os olen i 
sah . ee BaD EVE : a ¥ : 
Pi 4 4 a . 
* WV = 
2ax-|- a? 
- ot lomemeee A q : : 
‘ Ne eet OALLS 
, ames { 
& aaa 
j roe 
& a me he le a 
& yr 
in £ & ee aaNet enti, erie ellen Ne mlirete ds ale gD | 
ate Fs 
Pen. 
ae ee ‘ 

) om ~ : i 
artes Ge on } ~ > Ke 
ne & = wh y “ ig wi had ak. 03 

Cas . - “e Q 
oan ~ - > iy 
a | : e 
Ps eS a nd < PREZ rik’ 
Mpelbhics OPA A NN By ETS teens Oh artes tt yn a ON 
ro 
tee 
oa - ry 
. a -“ rd 


oat 


~MifceHanea Curiofa. 229 
PROP. Iv. THEOREM. 


Cg. 36.) The Space AGF contaiw’d an- 
der the Catenaria AF, and the right 
_ Lines FG, AG, parallel to AB, BF, 
boas equal to the Rectangle under the Se. 
- wmiaxis AC, and DH the difference of 
the Ordinates in the wich emai ana Ca- 
tenaria. 


ro ‘DH C= BH — BD = = by Prapofi 


ax-eeie an 
Coe Ths a aa se) 
| ae — V aaa-| x? | 
ex : : age : a 
ee. Wherefore the Eon of the 
ae 


Redangle under re given Line AC and DH 


wae ax 


bias RG) 


NE suse ea A Sige | ae 
= the Fluxion of the Space AFG. And 
fince thefe Figures do arife both together, it 
follows that the Rectangle under AC and 
pa. is equal to the pase 2 AGF. Q: E: dD. 


iQ + COROL 


— 


230 «©Mifcellanea Curiofa. 


EQROEL 


Hence it follows that the Space FAT 
comprehended under the Catenarsa and Hori- 
zontal Line FD, is equal to the Rectangle 
under FD and BA, lefs the Rectangle un- 
der cither Axis of the Hyperbola AH, and 
DH the excefs of the right Line BH or the” 
Curve AD, above the Ordinate BD. 


PROP. V. THEOREM. 


(Fig. 36.) If to the right Line AL Ge ap- 
plied the Reétangle LE, equal to the 
Hyperbolical Space ALH, then E will 
be the Center of Gravity of the Cate- 
navia AFD, | ; / 


Let the Curve FA be conceiv’d to be li- 
brated upon the Axis GL. Then (from the 
Doétrine of Centers of Gravity) it is mani- 
feft that the Afomentum of the ponderating 
Cvrve FA is expounded by the Superficies 
of an upright Cylinder erected upon FA, 
and cut off by a Plane, pafling through GL, 
and making an Angle of 45° with the Plane 
of the Curve. And the Fluxion of this Su- 


perficies or FA x FG, is equal to the Floxion 
. of the Space ALH or BH x HL; _ becaufe 
FA, BH, as alfo FG and HL, are equal. 

eae | une And > 


Nope Sh Tein 74 
Beene ae 
Bee Vl 
ri 


, Mifcelanea Curiofa. 131 
And confequently (fince they arife together) — 
the faid Superficies of the upright Cylinder 
is equal to the Hyperbolical Space ALH. 
Which therefore divided by the Pondus it 
f€lf AF, or its equal the right Line AL, gives 
the right Line AE, for the diftance of the 
Center of Gravity from the Axis of Libra- 
tion GL. So that the point E is the Cen- 
ter of Gravity of the Curve FAD, lying e- 

- qually on both fides the Axis. Q: E: D. 


COR OL: 


.. The Spaces ABHL, BAH, and AFG, are 
In Arithmetick Proportion. For the Fluxion 


Be i : Vi alee ol 
of the Space ALH is (= ——— ¥ X= 
V rax-|x? 


ax-l-x*%% = 2ax-\-a2? —ax Xx x 


— a ae oe 
MV roared? 2a x? 


——= 
ed 


i -— AX ie 
oF eee) = to the Fluxion 
, Vaax-bx? | 


of the Space BAH lefs the Fluxion of the 
Space AGF, by Propofition IV. And fince 
thefe three Figures do arife together, it fol- 
dows that BAH — AGF = (ALH=) BL— ~ 
BAH. Wherefore 2BAH = BL -| AGP. 

B 3H Q4 Whence 


+ Rae TS 
a 


232 Mife ellanea Cutiife. 


Whence ’tis plain that the Spaces BL, BAH, q 
and AGF, are in Arithmetical Proportion. 


COROL. Tl. 


| The Center: of Gite of the Bhinatia! 4 
is the Loweft of all thofe Lines that have ‘ 
the fame Termini, and are of the fame | 
length. For a heavy Body will defcend as 
far as it can, And fince the Figure it felf 
defcends as much as its Center of Gravity — 
defcends, ’tis manifeft that a flexible heavy | 
Line, will difpofe, it felf in fuch a manner, 
as that its Center of Gravity may be on : 
-er, than if it affum’d any other” ee 
And from this one Property of fach a Line, | ’ 
all the reft may ealily be hcber an; 4 


Ee OROL. Hf. 
If there be upright Cylinders ere@ed upon — ' 


any fort of Curves, that are of the famed 
length, and have the fame Termini D and F, 
with the Catexaria FAD; and thefe Cylind 
ers be cut by a Plane paffing through DF; 
then the greateft of all thefe Superficies thal 
be that which ftands upon the Catenaria.” 
For thefe Superficies (if the Angle contain’d © 
under the Planes he half a right one) divi- 
ded by the Curves (which in the prefent 
Gafe are all of the fame length) give the di- 
ftances of the Centers of Gravity from the 
right Line DP. And fince this diftance is 
greateft in the Catenaria <becaufe of the 

aay Defcent of the ‘Center: of Gravity) — 
| : therefore - 


— Mifcellanea Curiofa. 233 
therefore the Cylindrick ‘Superficies. fhall 
there alfo be greateft. Laftly, Becaufe the 
fame is to be faid of Cylindrick Superficies 
cut off by a Plane that make any Angle with 
’ the Plane of the Bafis, as is wheu the faid. 

Angle is half a right one; the Truth of | 
what was alflerted is evident univerfally. 


i 


LEMMA. 


Cig. 37.) Any Curve as AFQ, defirib'a 
. by the Evolution of another Curve KU, 
af apon any Ordinate, as FB (at right 
Angles to the Axis AB) be let fall per- 
pendicularly UR, from the corre{pondent 
Point U in the Curve KU; then (the 
Flaxion of the Axis AB continuing 
the fame) fball the Fiuxion of the 
Fluxion of the Ordinate BYE, the — 
Fluxion of the Curve AF, and the right 
Line FR be continual Pr oportionals, 


Let the Lineola Ff be produc’d ’till it meets 
the next Ordinate Wein oe And becanufe by 
the Hypothefis Fs = fw, alfo fhall of = Ff, 
and confequently oo fhall be the Fluxion of 
fs, that is the Flxion of the Fluxion of the 
Ordinate. Farther, the Triangles oo f, fFR, 
are Equiangular, becaufe oof = its "Alter- 
Maret ER, and. fog (Kir csi ER, bes 

caufe their difference R fr is as nothing in 
refpe&t of either of them, fince Rr is no- 


thing in refpeét of fr. And therefore oo: 


soa fF: FR; butef=fF, fince they oe 
er 


cs wie i mS vy ‘TPR ea, 


934 © ©Mifcellanea Curiofa. 
fer but by the Fluxion of either. There- 
fore alfoog:fF:: fF: FR. Q: E:D. 


- PROP. VI PROBLEM. 


(Fig. 37.) To find the Curve KV by the - 
Evolution of which the Catenaria ts de 
feribd. - eka 


x : i oe 
ES NESE SBT OE 


WS 


sae ie 


Let (as before) AB=x, BF=y. Then by 


te se ax Rane 
Propofition Il. j= eg Or 2axy* -|- 
Voaax-Lsce 


xxy? ar atx. Wherefore (by the Newtonian 
Method which now genérally obtains) aaxy? 
as ryy 2 ex y? -|-26 y (= oarws which 


~ becaufe of x = 0, fince the tconftant x has 


no Fluxion, is) =¢. Therefore y = : 
Seca axy — LY a-|-2x pg 


ae 
map 


2ax |e 2ax-|-% Ae open 
| | | V rax-bex 


CR Te 


ee go CR 
| Mh aan | gags 


(For the Sign — before the Quantity Y% de- 
| ~ notes. 


putting inftead of y its Value 


j 
es eRe eee 


Ser sidnly. 9 9." a es 
Rens BPA as 


— Maifcellanea Curtofa. 225 


-- notes only the place of the point R, with — 


refpect to F, to be oppofite to the place of 
the point F, with refpect to B, when the 
Curve AFQ is concave towards: the Axis 


testi 

AB.) And Ff (by Prop. i) =--—- : 

es | has oe 

Wherefore (by the foregoing Lemma) FR = 

(== abe xx? 2ax[-xx x V aax-L-sw 
ONY 2ax--xx a-l-x x ax? 


ap CERESET 


« V2an-ae, Again, becaufe of 


ae) a-|-x 
a 

the Rectangular Triangles Fs f, FRU, ha- 

ving the Angles f Fs, UFR, equal to one 

another (becaufe UFs is the Complement of 

either to a right Angle) we have Fs: sf:: 


a 


axe ah xV aan--xx 
FR: UR,or+: mes ee 
a 
/ 2ax{-xx 


UR, which therefore is = 4-|-x. Therefore 
_ the Nature of the Curve KU is fuch, that if 


panes 0 Pe 


a-|-x x V/ 2ax\-2xe 


: AB = *, FR fhall = er and 
| 3 a 
UR =a}x. Q: E: I 


COROL. 


Ra M. efeelanen Curiofa. 
| COROL. E- 
“AC: CB:: BH: BH: FR. poe this is 


the Property of the right Line FR, fe was: 
found juft tow. 


COROL. Tt. 


The right Line CB is = the nen Line 


Bl or UR. For each is = a-|-X- 
“CORO LTHEG jaa 


The Evoluent Line UF is a third Propor- 


tional to AC and CB. For becaufe of the 
fimilar eid fis, UFR, it iss F: F f 


palin fos 


Pua 3 © 


: FR: UF ; ore: 


(et Preenag J 


Vi2as-t-xe | 


—=—eSe 


a-\-% x ‘/ 3 AX-\-2N 


et 


at 


y 


[x | 
<= ———-, Whence a: a-\-x: f atx: UF 9 


phick | is the Radius of the Circle that has 


the fame Curvature with the | Capenanis at the 
eee F. 


COADL. 


——: UF, which is therefore 


¥ 
ee 
tea 
$35 
ca 


| Mifeellanea Curiofa. 237 


COROL. IV. 


‘When the point F is in A, or when the 
Vertex is defcrib’d by the: Evolution, that i is, 
_ when x =o, then the Value of the Evoluent 

_Line (or the Radius of the Curvature) UF 


(which in this Cafe coincides with KA) viz. 


Zz 


ae 


» becomes only 4.~ That is, the point 
a 

K where the Curve UK meets the Axis, «1S 
as ‘much above the Vertex of the Catena A, 
as C is below it. Whence the Diameter. of 
the Catena at the Vertex, — ‘is equal to the 
Axis. of the Conterminal Hyperbola. AH. 
And confequently the Cateza AD and the 
Hyperbola AH, have the fame Curvature in 
the Vertex A. For it 1s known that the 
foremention’d Circle has the’ fame Curva- 
ture with the Equilater: al Hyperbola AH, in 
the Vertex’ A:° But ‘this follows alfo. from 
the Property ofthe Catenaria, demonftrated 
at Rropefitian Ihe For the Nafeent PH Or CAP 


= the Nafcent BP —) \ eee is double the 


Nafcent BH or (V 2ax-L ae, that is, xv va- 
nifhing, when x is very fmall) /24x. And 
therefore the fame point is as well in the 
Nafcent Fyperbola, as in the’ Nafcent Czre- 
naria,.that is, the.one is coincident with the 
other at their firft arifing, and confequently 
thefe Curves have the fame Curvature at the 
erat ECe ae alten 


ss ae VS RHEE R OT. 


Saar A BN oat ye 


gaunt iy PART PSE Rees A gy ae Ten tt IL BHC RM CRON IL to” SOP a me ea (ve tALY a) ~ SS STIPE hth Sieg ERP Ps AP ae a Te 


See Mifvellanea Curiofa. Ee 


0 ctl pina EOE 


COROL. V. | 

The Curve KU is a third Proportional to 

the right Line AC, and the Curve AF or the ,. — 

right Line AL. For from the Property of 
the Evolution, KU = (UKA—KA=VF— 


ax a? —|-2ax—x? 


a a 


ae 2. And therefore, 4: V xax-fe i : 


V xax-Lex s. KU. But (by Cor. IL Prop. II.) 
V 2axlacx — AF. ‘Wherefore AC: AF-:: 


AF: KV. 
eras COROL VL 

‘The right Line KI is double of AB. For 
fince Bl = (BC =) CA-+AB, alfo Al fhall 
— CA-}2AB. But AK=AC)(by Gor. IV. of 
this Propofition.) Therefore KI=2AB. 

3 COROL' Vil. ) 

The Reétangle ACxBR is = to double the 

Hyperbolical Space BAH. For FRxAC = 


(apex V2axfwx “Zz a-t-x« Nf 4 ake) tee inca 
: a : Tits » 


+ 


xXx een xx ax A) Sicse ies = ABx BH 
: . --AC 


Maifcellanea Curtofa. 229 
-|-ACx BH=) ABx BH-|-ACx BD-+-ACx DH. 
Wherefore FRx AC—BDx AC (thatis, BRx 
AC) =ABxBH--ACxDH. But (by Propo- 
fition1V.) ACXKDH=Space AGF. Therefore 
BRx AC= (ABHL+-AGF= by Cor. |. Propo- 
_ fition V.) 2BAH. | 


PROP. VI. THEOREM. 


(Fig. 37.) If iz the Logarithmical Curve 
LAG (whofe Subtangent HS, given, w 
equal to the Line a, determin’d as at 
Cor. II. Prop. II.) be taken the point 
A, whofe diftance AC from the Alymp- 
tote HP, is equal to the Subtangent 
HS; and from the points H, and P 
(taken at Liberty in the Affymptote, 
and equally diffant from the point C) 
be erected the Lines HL, PG, Ordi- 
nates to the Logarithmical Curve, the 
half Sum of which is equal to HD or 
PF: Then the points D and ¥, {hall be 
pofited in the Curve of the Catenaria, 
_correfponding to the right Line AC. 


Let AB be put = x, and confequently CB 
or DH the half Sum of the Ordinates HL, 
PG, will = --x. Let the half difference of 
them be put = 7; whence HL = 4-|-x-|-y,, 
and PG = a-+x«+—y. And fince from the Na- 
- ture of the Logarithmical Curve, CA isa 
mean Proportional between them, aa fhall = 

AA 


re 


240 © Mifcellanea Curiofa, 


at NAO US 


aa ve 2ax |X — Vy whence y V2ax-bow. 


Confequently HEL = a--x-|- V2ax-|-ax, and 


PG —aA —|- x ede eeeed ba Wherefore the 
Fluxion of HL, or lm, is 


. le eae 2ax-|-wx 

: Woe as : 
fimilar Triangles JmL, LHS, ’tis LH: HS::— 
lm: mL; whence mL or dd the Fluxion of 


And becaufe of the 


aX 


Lis EAE is, the Curve 


: NV) rax-[ox | 
AD, generated after the foregoing manner, 
from the Logarithmical Curve, is of fuch a~ 
Nature, that if the Axis be x, and its 


BOS is 


Fluxion xe, the Fluxion of the Ordinate : BD 


Ax 


ig’ hte See es ie ee Property of 
ere ae oa 


the Catenaria correfponding to the right Line 
a, as was demonftrated at Prop. 1.’ There- 
fore the Curve FAD defcrib’d as aboye, is 
this very Catenaria it felf. Q:E: Do 


a. 4 


‘ Maifcellanea Curiofa. me 


Pare OL LARTIES. 
COROL. Lo: 
As the Catenaria is defcrib’d by the help 


of the Logarithms, fo on the other hand, 
by the help. of the Catenaria (a Curve pro- ~ 


duced by Nature it felf) the Logarithm of 


any given Number, or rather of any given 
Ratio, may be found. As if, putting CA=1, 
whofe Log.=o; the Log. of the Number 
CQ, or of the Ratic between CA and CQ, 
were fought. Let CV bea third Proportional 
to CQ and CA, and CB the half Sum of CQ, 


and CV; then an Ordinate to the Catenaria 
from the point B, viz. BD, will be the Log. 


fought. 


COR OL. fl. 


Vice verfa, if giving the Log. CH or CP, 
the carrefpondent Number HL or PG, or 


the Ratio of HL to CA, or PG to GA, be 
fought. From H or D ere¢t a Perpendicu- 
lar meeting the Cateza in D or F, and in the 


Horizontal Line AR, take CR==HD or PF, 
or CB. And then will AR be the half dif- 


ference of the fought Lines LH, GP, as HD 


‘the half Sum of the Extreams leffen’d by 
: R 


or CR, is (from the above demonftrated Pro- 
perty of the Catenaria) their half Sum. For 
in three Quantities Geometrically Propor- 
tional, fuch as are HL, CA, PG, the Square of 


the 


242  Maifcellanea Curiofa. 7 
the Square of the middle Term, is equal to © 
the Square of the half difference of the Ex- — 
treams. And confequently CR-|-AR, and 
CR—AR, are the Numbers HL or GP, 
agreeing to the given Log. CH or CP. 


COROL.: Fi. 


It is plain from the Demonftration, that 
as HD the half Sum of the Logarithmical 
Ordinates HL, PG, being applied at. right 
_ Angles to CH, is an Ordinate to the Care- 
naria, fo alfo the half difference of the fame 
HL, PG, applied at right Angles to CA 
in B, is an Ordinate to the Equilateral Hy- 
perbola, whofe Center is C, and its Vertex 
A; and confequently (by Cor. I. Prop. IL). 


<== the Catena AD. For y = MV aaie ves 
and fince it was fhewn in the foregoing Co- 
vol. that AR is alfo the half difference of — 
HL and PG; ’tis plain that AR is = the 
Portion of the Catenaria AD. From whence 
by the way, we may obferve a Method, how, 
from the Catena AD given, to find C the 
Center of the Conterminal Hyperbola, or 
the point in the Afymptote of the Logarith- 
mical Curve GL. For taking AR= the Ca-— 
_ tena AD, and joining the points B, R, from 
the middle of BR ere& a Line perpendicu- . 
lar to it, which will meet BA the Axis of 
the Catena produced, in the point C, fought. 


G | Which Is evident, fince thas CR will = CB. 


COROL. 


Mifcellanea Curiofa. 243 | 


BOR OLS IV. 


Hence alfo it follows that if the Angle 
BDT be equal to ACR, the right Line DT 
touches the Catenaria in D. For then it will 
be (in the fimilar Triangles DBT, CAR) | 
ie. bes. CA: AR, of CA: Cutve AD 
which is = AR. And confequently DT 
touches the Cutenaria, by Corol. Prop. I. 


QOROL: ¥V. 


It follows alfo that the Space ACHD = 
the Rectangle CAxAR. For becaufe (by 
Prop. IV.) AYD=CAx (AD—BD, —=AR— 
AY, by Cor. III. of this Prop. —) YR; the 
thing is manifeft. And fince CA is given, 
*tis plain that the Space ACHD is as the 
Curve AD, and the Fluxion of the former 
Hd, as the Fluxion of the Latter Dd. 


COROL. Vr 


__ If through the point K where CR cuts HD, 
we draw KZ parallel to PH, meeting AC in 
Z, and tdke CE = eee 3 then will E be 
the Center of Gravity of the Curve FAD. 
Imagine an upright Cylindrick Superficies 
erected upon FAD, and to be cut by a 
Plane pafling through PH, and making an 
Angle of 45 with the Plane of the Curve 
FAD. This Superficies, will expound the 
x hoa R 2 Momen= 


2 oy ee ee ae 
ee a 3 


244 — Mifcellanea Curiofa. 
pa ee of the Curve FAD librated on 
the Axis PH; an@¥its Fluxion is DHxDd-\- — 


axe 
PF x Fi=2BCx AD=3a p28 \-24 x — = 
| Miata < 
2a? pa Saw |- 22a wae 
Gerpcemm nese OS eee Teese Gees Ey 
V 2AK-|-X Vaart [-w3e 
a* x-|-axee Zaxxl-2e? x 


-|-——-_---—-; the Fluent of 
ee a Vague! 


Which, ax BD-- av 2ax-|-xx-|- aN sax = esi 
‘CAxBD-| CBxAD. Wherefore CAxBD-|- 
CBx AD= (Cbecaufe it arifes together with 
it) to the foremention’d Cylindrick Superfi- 
cies— the Momentum of the Curve FAD 
with refpect to the Axis of Libration PH. 
Whence the diftance of the Center of Gra- 
vity of the Curve FAD from the ee C, 

is CAxBD-} CBx AD 4 1 CAxBD - 

QADa rut oa y ADanom 

Farther, becaufe of ZK. parallel to AR, tis 
AD: BD:: (AR: ZK: :) CA: CZ, whence 


GZ — CAxBD 4 and therefore CE which by 
Conftructiion is = 3 BC-|- 3 CZ, ‘fall oa 
aige +-2BC. That is, the Center of 


| Craig of the Curve FAD, and the point E 
: determin’d 


| Mifcelanea Curtofa. 245 
determin’d by this Conftru@tion, are equally 

diftant. from the point C. But they are alfo 
pofited in the fame right®Line, and towards 
the fame parts, and therefore they coiacide 
with one another. This G@oincidence of the 
point E as determin’d above, with the Cen- 
ter of Gravity as found at Prop. V. may be 
thus /ysthetically fhewn. By Cor. I. Prop. V. 
2BAX = AYD-|- BAx AR. Whence AH -+ 
2BAX = (ACHD -|- BAx AR = by Cor. fore- 
going) ARxCA-\|-BAxAR;3 that is, BDx 
AC-|- 2BAX =ARxCB; or BDx AC = AR 
xCB—2BAX. Whence BDxAC-|- ADx 
BC= (ADx BC -\- ARx CB — 2BAX = 2AD 
xBC—-2BAX =) 2ADx AC -|- 2ADx AB — 
2BAX. And-dividing by 2AD, we have } 
VEDY AR inn rac |: ABKXAD—BAX 

AD |-z BC = (AC-| aan = 
CA -|- pee But ee is the diftance of 


| ARS AR 

the Center of Gravity of the Catexa from the 
Vertex A, determin’d at Prop. V. and confe- 
quently, according to the 5th Propofitiow CA 


wats ete is the diftance of the point EB from 


BD 7 
C; now 2 shies -|- 3 BC, is the diftance 
of the point E alfo from the fame point C ac- 
cording to thisCor. Whence’tis manifeft that 
thefe two Determinations of the point EB 


; X 
amount to the fame; becaufe CA -|- a = 
1 BDx AC 4456. 


aes ie | a 
pore aial > ae ae COROL. 


hd 


246 “Mifcellanea Curiofa. ‘ 


CORMOL. VIL 


~The Center of Gravity of the Space 
PFADH, is in I the middle point of the 
right Line CE. For fince the Center of 
Gravity of the Fluxion of AD, or Dd, and 
Ff, is twice as far diftant from PH, as 1s the 
Center of Gravity of the Fluxion of ACHD, 
or DHhd, and FPpf; and Dd-+-Ffx AC 1s = 
DdhH-\-FfPp; ’tis plain that B, the Center 
of Gravity of the Fluent FAD, is twice as 
far diftant from PH, as I, the Center of 
Gravity of the Fluent PFADH. But this 


~ may be yet fhewn otherwife according to the 


Method us’d before. Imagine an upright 


‘Cylinder to be -ere&ted upon the Figure 


PFADH, and to be cut off by a Plane paf- 
fing through PH, and making an Angle of 
4§ with the Plane of the Bafis. This Solid 
will expound the AZomextum of the Figure - 
PFADH librated on the Axis PH. And 
the Fluxion of this Solid or A¢omentum (viz. 
the Solids erected on the Bafis PFfp, and 
HDdh) is produced, by multiplying the A@- 
mentum of the Fluxion, or the Fluxion of 
the Atomentum, into ; AC given. For by 
Cor. V. of this Propofition HDdh=Ddx AC, 
Wherefore the Fluent Adomentum it felf, is 
produced by multiplying the Alomentum of 
the Curve FAD with refpe& to the Axis 
PH (as determin’d at Cor. foregoing) vz. 
CAxBD-|-CBx AD into ; AC; which will 
therefore be  ACx ACxBD-|-4ACxCBx AD, 
Aud confequently if this be divided by the 
a pes le Oe ee librated 


ie The *, . 
4 
\ 


~~ 


CO Mifcellanea Curtofa. 247 


librated Figure PFADH (=2CAxAD, by 
Cor. V. of this Propofition) there will arife 


(for the diftance of the Center of Gravity of 


the Figure PFADH from the Axis PH) 4 
CABID HL 2 
Za -|-4 CB 5 which. 1s — 3 CE. deter- 


min’d above. ; 
Pee OR OL, VII. 

If through the point N where DT the 
Tangent to the Catezaria in D, cuts the 


Line AR, be drawn a Parallel to BC, meet- 
ing in O a parallel to AR drawn through E ; 


then will O be the Center of Gravity of 
the Curve AD. For by Cor. 6. the Center 


of Gravity of the Curve AD is in the right 
Line EO. But it fhall be demonftrated to 
be in the right Line NO ; and confequently 


‘that O it felf fhall be the point. Let DA 


be conceiv’d to be librated upon the Axis 


HL; then the Afomentum of this is the 


Curve DA multiplied into the diftance of 
“the Center of Gravity from HL. And 


wity) = Waar lex K ee 


confequently its Fluxion = DA x Hh (Hh 
being the Fluxion of the diitance of the 


Axis of Libration from the Center of Gra- 


ax 


—=ax. -And 


| MV 2ax-|-x? 


| therefore the omentum of the Curve DA, 


with refpec to the Axis HL, is—= 4x. And 
-confequently the diftance of the Center of 


Gravity from the fame Axis, is 2x divided 


R 4 by 


& 


“~ 


248 Mifcellanea Curiofa. 
by AD, or SAO But becaufe DT - 


touches the Catenaria, by Cor. 4. of this Pro- 
pofitien, the Angle BDT, or DNY=ACR, | 
and the Angles at A and Y are right ones, 
therefore in the Equiangular Triangles” 
RAC,” DYN,>. ’tis’ RAY AGr. Bae 7S 


whence YN = eee that is Yas, the — 


- diftance of the Center of Gravity of the 
Catena AD from the Axis HL; or that Cen- 
ter is in the right Line NO. i 


COROL IX. 


If through the point I be detera” a right 
Line parallel to AR, meeting ON produc’d © 
in W; then W fhall be the Genter of Gra- 
vity of the Space ACHD. For by Cor. 7 
the Center of Gravity of the Space ACHD, 
isin the right Line TW, but it fhall be de- 
monftrated alfo that °tis in NW, and confe- 
quently W is the point. For (after the 
fame manner as in Cor. foregoing) the Fluxion 
of the Afomentum of the Space ACHD ponde- 
rating upon the Axis HL, will be fhewn to be 


(ACHDx Hh=ACx ADx Hh= =) Aa 


aX 


= ax. And confequently the — 


Vax} foie : 
Momentum of the Space ACHD, with re- 
{pect to the Axis HL, is the Fluent of this _ 

“Fisxion, 


— Mifcellanea Curiofa. 249: 
Fluxion, az, that is, 27x. This therefore 
divided by the Space ACHD, or 


ee gives the diftance of the 
_ Center of Gravity (of the Space ACHD) 


| ; Be 
from the Axis HL, which is = — 


le luxe 


- And therefore the Center of 


- BGs DY 
PS CAR 

Gravity of the Space ACHD, is in the Line 
NW. And fiom thefe two laft Corollaries, 
is found the Center of Gravity of any Por- 
tion of the Catena, though not reaching 
the Vertex A, or alfo of any Space com- 
prehended under any Portion of the Cate- 
maria, and any other right Lines befides 
thofe aforefaid. 


z= 


COROL.. X. 


Hence are meafur’d the Surfaces and So- 
lids generated by the Rotation of the Ca- 
tena (or a Space comprehended under it, 
and a right Line) about any given Axis. 
For a Figure generated by fuch a Rotation, 
is (as is vulgarly known) equal to the gene- 
nerating Figure multiplied into the Periphe- 
ry defcrib’d by the Center of Gravity in the. 
Rotation, which Periphery is given, fince 
the Radius or Diftance of the Center of 
Gravity from the given Axis, is given. Thus 
if the Catena AD roul’d about the Axis oo 
as ined Aa 


aso © Mz fcellanea Curtofa. 
then a AN is the Periphery deferib’d by the 


Center of Gravity O oF denoting the Ratio 


of the Periphery of a Circle to the Radius) oy 
and confequently the Surface generated by 


the Rotation of the Catexa AD = Fx 


ANx AD=) ~ x ANx AR. That is a Cir- 


cle, the Square of whofe Radius is double 
the Rectangle RAN, will = the Surface ge- 
nerated by the Rotation of the Catena AD 
about the Axis AB. After the fame man- 
ner the Solid generated by the Rotation of 


the Space ACHD about AC, may-be fhewn ~ 


- to be equal to a Cylinder, whofe Bafis is the 
foremention’d Circle, and its Altitude=AC. 
_ Thus alfo the Surfaces and Solids produced 
by the Rotation of thefe Figures about any 
other given Axis, are meafur’d. For givin 
the Center of Gravity, they are eafily dif- 
coverd. | : 


Of 


—Maifcellanea Curiofa. - 251 


Be Of the Quadratures of Geometri- 
cally wratinal Figures. 


By J. Craig. 


- ET ACF (fig. 38.) be a Semicircle, 
whofe Diameter is AF, ADE a Geo- 
metrically irrational Curve, whofe Ordinate © 
BD cuts the Semicircle in C. The Quanti- 
ties may be noted thus; The Diameter AF 
=a, 100 Abicifle AR = y, the Arc AC = 
v, the Ordinate BD =<: And let 2 =rvy” 
a General Equation exprefling the Nature of 
the Geometrically irrational Curves ADE, in 
which rv denotes any given and determin’d 
Quantity, and # an indefinite Exponent of 
the indetermin’d Quantity y. I fay the Area, 


: roy cata 
ABD = — qv-[ V aay — yy x 
ra 2nra® —\-ra® 
ee eee OP 
waht nx n-|-1| 
 AAX2I—t BX 2M —3 
: Ca a SOIREE rae si 
i—1 Pe 
ACK20—J AD 27i-—7 
— i— 
y" 4 -|- cemnenraccemanaman) J 5 
in—3 woth 


akE%x 2m 


252  Maifcellanea Curiofa. 
AEX 2N—9 | | 
ane 
In this Infinite Series, thefe things are to 
be taken notice of :*(1-) That the Capital 
Eetters A, B, C, D, EB, @e dencte theta. 


efficients of the Terms immediately pre- 


2nraa -\-raa 


B= 


‘ceeding them, wz. A= se 

ey eae aX n-\-1 Xn-|-1 
aAkin—1 aB%2n—3 - . at, 
, and foon. (2.) 


ete, OG 
a— 1 ND, 
That if the Exponent 7 be an Integer and 
-Pofitive, or equal to nothing, or if 2” be an 
odd Number, then the Quadrature of the 
Space ABD may be exhibited by a finite 

Quantity: The Seriesinthefe Cafes breaking 
off. (3.) That q denotes the Term laft break- — 
ing off (4.) That all thofe Figures in which ° 
the Series is broke off have one Geometri- 
cally Quadrable Portion very eafily affign- 
able from the Series it felf, vzz._if you make 
E I 


the Abtciffe yr *F!-[-ng} gl; there 
will arife a Geometrically Quadrable Areaan- 
fwering to this Abfcifle. (5.) That only the 


Irrational Terms V xay—yy is to be multi- 
tiplied into the Terms following it. 


E xample 


“Mien Cw | 252 


Example ¥ I. 
Let z= v, becaufe in this Cafe r= 1, 
| ra 
n=, therefore — is the Term laft 
n-\-1|? 


breaking off wherefore q = 4, whence ABD 


= vy —av-|-a V 2ay—y2: And confequent- 
ly if (by Note 4.) you take the Abfciffe 
y = 4, that is, if the Ordinate pafs through 
the Center of the Circle, there will arifea 
Geometrically Quadrable. Portion fitting it, 
viz. Area = a*, that is, the Square of the 
Radius. : 


i dann TI. 
¥ vy | ak 
Let z==—. Becaufe in this Cafe r — 
-2na* as ra? 
== 1, therefore —-— 
ny n—|~-1) a? 


d 


y"—* isthe Term 


| oe Le 
a breaking ot jes qg == —; whence 
rs os we E A 4 Z 


, es 3av yr a. 
Ae ay oo oT te 


Vay —y 2 and 
confequently, if uae Rote pe ‘you take 
y= RAE 39% there will arife a Geometrically 

) Quadrable 


284 Mife ellanea Curiofie. 
Quadrable Area fitting this Abfcifle, .viz. 


area = Vi Hide -|- oo 


Heal HHI. 
Let = a 


In this Cafe r= ; —-, Bk, 
aa 

; a 2i——T yoo ' 

therefore —————— _ y"? is the Term laft 

Yom] 

breaking off, therefore 7 = x : whence by 
Infinite Series, will ABD = 
6uy3—1 5a? v-|-2ay?-|- ‘3a y- _L1s oan 


EE NS NES Se 
ee 3 


18a? 
And confequently, if (by Note 4.) you take 


y= a/ i > there will arife a Geometrically 
Quadrable Area fitting this Abfcifle, viz. 
aay" -|- 5a 'y rh 15a? | 


te 


x aay sae y? 5 


Area = 
184 


Secondly, Let ACF (Fig. 39.) be a Pow 
bola, AE its Axis, A the Vertex, and (Ba) 
the Latus Reftum. And let. ADG bea Geo- 
metrically irrational Curve, whofe Ordinate 
BD cuts the ParabolainG. Let thé Abfcifle 

AB= y, 


— Maifcellanea Curiofa. 255° 
AB =y, the Ordinate BD = z, the Arc of 
the Parabola AC =v. And let the General 
Equation exprefling the Nature of Infinite 
irrational Curves be this, Z = rvy”, in which - 
_ry denotes a given and determinate Quantity, 
and z an indefinite Exponent of the indeter- 
mind Quantity y. I fay the Area 


alt prea 
wet) ese qu -|- V aay ye 
i n-\=1 2 
ag n-\-t ad a ne 
n-|-2X%2-|-4 p-oxnl1 2) 


Reg pt SARIN! yaa 
nx n-|-2Xn-|-11 3 See ! 


' ABR Ii—3 yy 9 AC KIN—F§ 
eee ag 


In this Series ’tis to be noted: (1.) That. 
the Capital Letters A, B, C, cc. denote the 
- Coefficients of the Term preceding them. 
(2.) That if the Exponent z be an Integer 
aad Pofitive, or equal to nothing, or if 27 be 
an odd Number, then the Quadrature may 
be exhibited by a finite Number of Terms; 
the Series in thefe Cafes breaking off. (3.) 
That--|- ¢ is equal to the Term laft breaking 


. off (4.) That of the Terms multiplying the 


Quantity VV 2ay -\-y?, the laft breaking off is 
to be doubl’d. (5.) That all thofe Figures 
in which z is an Integer, Pofitive and an odd 
Number, or more generally, all thofe Fi- 
gures in which the laft Term kaa hind 
: as 


956 © Mifcellanea Curiofa, — 
has an Affirmative Sign or+|-, have one — 
Geometrically Quadrable Portion, and aflign- 
able from the Series it felf, by taking the 
Ab{fcifle as in the fourth Note of the pre- 
ceding Series. | mete? s 


Example d.° 


‘Let z — v, becaufe in ‘this Cafe r 4; - 
n—o, therefore the Term laft breaking off 
is — a es whence -|-4 = (by 
n-\-2.%0-|-1| . 


Note 3.) and becaufe in this Cafe —<= is 


the laft Term to be multiplied into V 2ay—y, 


fem ES 


therefore ABD = vy -|- - 2 V aay |; y7 x 
mii y mm Ae ee | 


Example Xt. 


U _ ; ! I 
Let z= a becaufe in this Cafe r= —, 
a 


m == 1, therefore the Term laft breaking off 
Ze Aa hese 
aah Ato Ay cilia * , whence g=4 4, 
nxn-|-2xn-|-1| ~ % 
and 4 z is the laft Term to be multiplied by 
V 2ay-\-9?, therefore | | 
ABD 


iM — Cori Q 5 7 


A aa : “Sa 
ABD = : oa aa yx ra 


ce E+“. And if you take y= V3 aa, 


there will arife a Geometrically Quadrable- 
Area rea fitting — oe Abfciffe, viz. Area = 2, 


i a ea a - x aa V0? : 


a I have shes Theorems of this Nature, 
for Figures depending on the Circle and Pa- 
rabola; but thefe two may fuffice as a Spe- 
cimen to fhew the Ufe of my Method pub- 
lif’'d in my Treatife of Quadwatures, in de- 
termining the Quadratures” of Irrational Fi- 
guges, for which there has been no Method 
(as far as I know) as yet made Publick. 


That the Reader may the more eafily 
come at the Invention of thefe and the like 
Theorems, I fhall fubjoin another, and more 
hereafter, ‘if need be. | 
- Let therefore (Fg. 40.) ACE be! a Se- 
micircle, ADE a Geometrically Irrational 
‘Curve, whofe Ordinate BD cuts the Semi- 
circle in C. Let the Quantities be denoted 
as before, wiz. the Diametér AF = 2a, the 
Abfcifle AB = y, the Arc AG = 4: the Or- 
dinate BD =<} and let z = rv 27, an E- 
quation exprefling the Nature of the Curves 
‘ADE, in which r denotes any given and de- 
termin’d Quantity, and # an indefinite Ex- 
‘ponent of the indetermin’d Quantity xT 
fay the Area’ * 
| $ ABD 


258 Mifcellanea Curiofa. 


242-\-1 , i. 
- ABD = fe qu* -\-v V sayy? % 


Leal | 


——2 : Paes “|- 
n-\-1 | nkn-|-1| 
AA, itl yy aby by ere T 
ma yt 2 Sie ——___—+ me ed 3 =. 
career I——-2, 


ACK 2-5 aDKX2n—7 : 
ins POT 4.| yt - 54 


(gan Oe eas 
AEXUM—9 yb 9. ie 
mere MNS 


m-\-11 


ara R2n|T yg a? AK IH—T 


n~a1 fd 
gl RAPES OAT 390 <8 Cae ae 
mt xn-\-t| FBS 
2 2f,. tT gs 
A” BY LMm—3 op ae ik Beh) eee ee 
eG eat 7 Sy a eae 


on Ome? 


; 


In ‘this Theorent thefe Things are to be 
taken notice of; C1.) That ’tis. made up of 
two Infinite -Series,. the former of which 
(connected by the Sign -|-) is.multiplied in- 


to v V sayy? ; but the Terms_of-the latter 
(affeGted, by the Sign.—) are Abfolute. (2.) 
_ That in the. former Series, the Capital. Let- 
ters, A, B, C, @c. denote the Coefficients of 
the Terms refpectively preceding them, and 
m the latter have the famg Values as in the 

is * Tae ’ former 


ie load Curiofa. 2 : 9 


Merci (3-) That the Quadrature may be 
exprefs’d by a finite Quantity, when » is a 
pofitive Integer, or equal to nothing, or if 
22 be an odd Number; for in thefe Cafes 
each Series is broke off. (4.) That 29 is 
equal to the laft Term breaking off, of the 
former Series. 


Example I. 
uv” : a 
het =. Becaufe in this Cafe x =o, 
a ae i. 
Fis s, therefore fhall the Area ABD = 
v?-|-2Y V ray—y?—24). 


COROLLARY. 


The witole Figure AFE is equat to twice 
the Square, whofe fide is ACF, lefs the 
Square of the Diameter. 


Example A. 


Let rl becaufe id this cae n= T; 


i et deste ‘al dhe! Area ‘ABD = = 


pen 
ie 


blvow. | i e yu? 


460  Mifcellunea Curiofa. 


ual Pe ae aA Bo i y ae Ly? 
aa" ta” — LT Seria 
ey, 
a* 


Example Il. 
yo Ne ‘ . 
Letz =>, becaufe in this Cafe # = 2, 


I 
a> 


c= 


B 2 
, therefore fhall the Area ABD =" 


= 
Nr ners: 


a ye ee eee 
ies 


oy) STs ee 
274. 2.18 3 


While I was writing this, I receiv’d the 
late Months of the Lipfick A&s, mn which L 
read, with a deal of pleafure, feveral excel- 
lent things for promoting Geometry; and 
among them fome Remarks of Mr. Lezbuitz, 
and Mr. ¥. Bernouili, upon my Method of 
Quadratures. - In the its of April, An. 1695. 
Mr. Lecbnitz informs us that he has a Me- 
thod fomewhat like ours; and truly, I migh- 
- tily Congratulate my. felf, that any thing of 
mine could have the leaft likenefs to the 
Thoughts of fo great-a Geometer. But 
whereas he fays his own is much more Ge- 
neral, and fhorter than mine; I make no 
doubt of that. It were to be wifh’d, he 
ee ge would 


— MifceHanea Curiofa. 261 
would no longer fupprefs this Method of 
his, and feveral other things he has, efpe- 


cially relating to his Differential Calculus, but 


rather, as foon as his Leifure permits, pub- 
lifh them for the Good of the Common- 
wealth of Learning. In the mean while we 
hope the Illuftrious Marquefs De PHofpital 
will fpeedily make publick what is neceflary 
to perfe& that Calculus, in the latter part 
of that excellent Work of his, which Gn 
the Preface to the former part) he informs — 
us, he has compos’d upon the Integral Caleu- 
lus. We expedct.alfo, with fome Impatience, 
that other Section, in which that Noble 
Author promifes he will fhew the Ufe of 
his Calculus in Phyficks and Adechanicks. For 
whatever he has publifh’d, as well thofe 
Specimen to be found featter’d in the Lip- 
fick Aéts, and elfewhere, as that excellent 
Book of his CIntitul’d, <Axaly/e des Infiniment 
petits) caufe us to expeé great Things from 
that Noble Marquefs. ae 

Whereas the Ingenious Mr. . Bernouslls has 
thought fit Gin the Acts of. February and Au- 
guft, An. 4695.) to fay my Method is not 
General, I freely confefs it, as that Saga- 
cious Perfon might eafily perceive in the 
 Courfe of my Examples. In a Matter fo 
Intricate I took what Steps 1 could; and if 
deter’d with the length and difficulty of the 
Journey, I then made no farther Progrefs. 
I might fairly make a Step where I pleafe, 
fince my Application to thefe Mathemati- 

cal Studies,is only by the by. Mr. Bernouiiti 
has partly hinted where my Method is at a 
sot 3.3 Stand, 


262  Mifcellanea Curtofa. 
Stand, though he feems not to have taken i 
up the whole Matter. In the mean while — 
J acknowledge my felf ‘highly oblig’d, that — 
he has honour’d my Treatife with his Ani- 
madverfions; but much more fo, that he - 
was willing to free me of my Miftakes, 

with fo much Candor and Humanity. : 


ore ie 


a“ 
Do a 
ca eR tng tC 
4 : - 
i 


Ba oy ager ie in Re 


2 ES ame 


Ss eee oe 


— Zoos 


he) 
a raen 


M ifcellanea Curifa. 262. 


Concerning the apparent Magnitude 

fs of the Sun and Moon, or the ape 
rent diftance of two Stars when 
mgh the Horizon, aad when 
higher elevated. | 


| if Do not defign fo much to eftablifh any — 
_ thing of my own that may be fatisfactory 
in folving this admirable appearance, as to 
_ dete& the Errors of thofe that have offered 
at a Solution thereof, and have come fhort 
(as I conceive) of being fatisfa@tory ; that 
thereby I may again fet the minds of Philo- 
fophers on work, and roufe them up to en- 
quire anew after this furprizing Phexomenon. 
That I may do this the more effectually, I 
_fhall briefly declare the Matter of FaQ, and 
_ then proceed to the Reafon thereof, given by 
-feveral, and to their Confutations. 
Firft therefore itis well known that the 
mean apparent Magnitude of the Moon is 
30 m. 30 f. we will take it Numero Rotundo 
to de 30, that is, an Arch of a great Circle 
in the Heavens of 30 Minuts 1s covered by 
her Diameter; and this we'll fuppofe ta be 
her apparent Diameter, at a full Moon in the 
midft of Winter, and when fhe’s in the Me- 
ridian, and at her greateft Northern Lati- _ 
tude, and confequently the utmoft that fhe - 
can be elevated in our Horizon; ’Tis as well 
bird | eS a Known 


264 Mafcellanea Curiofa. 
known alfo that when fhe is in this pofture, 
being looked upon by the naked Eye fhe ap- 
_ pears (that we may accommodate all to fen- 
fible Meafures) to be Magnitudims Pedalis, 
about a foot broad. But the fame Moon be- 
ing looked upon juft as fhe rifes, fhe appears 
to be three or four foot broad, and yet if 
with an Inftrument we take her Diameter, 
both in one pofture and t’other, we hall find 
that ftill fhe fhall be but. 30 Minutes; the 
feveral ways of trying this I will not mention, 
they being as various as are the Methods of. 
taking the Moons apparent Diameter, com- 
mon enough among the Aftronomers , neither 
will I infift upon the truth of the Matter of. 
Fad, for that I think cannot reafonably be 
queftioned, after fo many trials and fo many 
experiments thereof, faithfully recorded by 
undoubted Witnefles; and it would be very 
unreafonable to imagine that fo many Au- 
thors fhould rack their Brains for folving an 
appearance wherein they were not certain 
of the matter of FaG@. But becaufe of Wul- 
“lius in Verba, ¥ can affert that I have ac- 
curately try’d it my felf, and I have fo 
found it: One of the ways I proceeded was 
thus; I took avery good Telefcope of about 
6 foot long, in the inward Focus of whofe 
Bye-Glafs | apply’d a very fine Lattice made 
of the fingle hairs of a Man’s Head; then 
looking with this at the Moon when fhe was 
juft rifen and looked extraordinary big, I ob- 
ferved what number of the fquares of the 
Lattice were occupy’d by her Body ; then ob- 
ferving her again, when more elévated and’ 
free from all extravagant Greatnefs, I ftill 
bE £ yee = ' Faia * 3 ee A eh r: found 


Mifcellanea Curiofa. 265 
found the fame fquares of the Lattice pof- 
- feffed by her. This way is equivalent to that 
now more ufed, of taking her Diameter by 
Mr. Townly’s Micrometers, but I have alfo 
tried and found the fame thing by an accu- 
rate Sextant, taking the diftance of the 
Moons oppofite Limbs. ; 

Now this Phenomenon affords two things to 
be confidered, firft why the Moon (I ftill 
name the Moon as being an Objeé& more 
adapted for our fight , for the fame thing 
holds in the Sun) fhould feem bigger about 
the Horizon, then when more elevated ; and 


-_ fecondly, fhe appearing bigger, how comes it. 


to pafs that her Diameter being taken, it is 
no greater than when fhe appears lefs. But 
the Difquifition concerning this latter being 
likely to comprehend the former, | fhall not 
divide my Difcourfe into two Branches, but 
proceed in the Method propofed. Only I 
defire it may be noted, that I fuppofe-the 
Horizontal and Meridional Moon to be found 
both of the fame Angle, whereas in truth the 
the .Meridional Moon (tho’ appearing lefs) 
fhall be found of the greater Angle: which 
increafeth the Wonder. But this proceeding 
from the different diftances that one and the 
other is looked at (the Meridional Moon be- 
ing nigher us by almoft a Semidiameter of the 
Earth) and confequently eafily folved that 
way; I havetherefore chofen to put hetween 
them a plain equality, for avoiding Coufufion 
and Intricacy in Difcourfe. 
| Wherefore let us hear what the Ingenious 
_ of thefe latter days can fay to this appearance. 
And firft we find the Celebrated Des-Cartes at- 
oo tributing 


266 Maifcellanea Curiofa. 
tributing this appearance rather to a deceived 
Judgment than to any Natural Affe@tion of 
the Organ or Medium of fence; forthe Moon 
(fays he) being nigh the Horizon, we have a 
better opportunity and advantage of making 
an Eftimate of her, by comparing her with 
the various Objects that incur the fight, in its 
way towards‘her; fo that tho’ we imagine 
fhe looks bigger yet ’tis a meer deceit; for 
we only think fo, becaufe fhe feems nigher 
the tops of Trees or Chimneys or Honfes or 
a fpace of Ground, te which we can compare 
her, and eftimate her thereby ; but when we 
bring her to the Teft of an Inftrument that 
cannot be deluded or impofed updn by thefe 
appearances, then we find our Eftimate 
wrong, and our Senfes deceived. Thefe 
Thoughts, methinks, are much below the ac- 
cuftomed accuracy of the noble Des Cartes ; 
for certainly if it be fo, I may at any time in- 
-creafe the apparent bignefs of the Moon, tho’ 
in the Meridian; for it would be only by 
getting behind a Cluiter of Chimneys, a Ridg 
o: a Hill, or the top of Houfes, and compa-~ 
ring, her to them in that pofture, as well as 
in the Horizon, befides if the Moon be look’d 
at juft as fhe is Rifing from an Horizon de- 
termined by a fmooth Sea, and which has no 
more Variety of Objects to compare her to, 
than the pure Air ; yet fhe will feem big, as 
if lookt at over the rugged top Of an uneven 
Town or recky Country. Moreover, all va- 

riety of adjoining Objects may be taken off, ~ 
by lookiag through an empty Tube, and yet 
the deluded imagination ts not at ‘all helped 
thereby. Icome next to the folution hereof 
: Mee | given 


Mifcellanea Curiofa. 267 


given by the famous Thomas Hobbs, and for 


this we fhall ftand in need of Figure at. 
wherein, fays he, let the point G be the Cen- 
ter of the Earth, and F the Eye on the fur- 


- face of the Earth ; on the fame Center G let 


‘there be ftruck the two Arches, EH deter- 


mining the Atmofphere, and A D to repre- 
fent that blue furface in which we imagine 
the fixed Stars; and let FD be the Horizon. 


‘Divide the Arch A D into three equal parts 


by the lines BF, C F, it is manifeft that the 
Angle AFB is greater than the Angle BFC, 
and this again greater than the Angle CFD. 


‘Wherefore fays he, to make the Angle CFD 
equal tothe Angle CPD, the Arch CD mu 


be greater than the Arch CB ; and confe- 
quently, that the Moon may in the Horizon 
appear under the fame Angle as when ele- 
vated, fhe muft cover a greater Arch, and 
therefore feem greater; that is, the Moon 
in the Meridian appearing under the Angie 
BFC, that fhe may appear under an equal 
Angle in the Horizon, as fuppofe CFD, ’tis 
neceflary the Arch CD fhould be greater than 
CB; and confequently tho’ fhe appear to ful 
tend a greater Arch when in the Aorizox 
then when elevated, yet fhe appears under 
the fame Angle. And all this without Re- 
fraction. The Geometry of this Figure is 
moft certainly true and demonftrable. At 
this I quarrel not ; Lut it makes no morein 
our prefent Difficulty than if nothing had 
been faid ; for the Philofopher has here made 


a Figure of his own, and from thence he ar- 


gues as confidently, as if Nature would ac- 
commodgte her felf to his Scheme, and he 
a A net 


265 Mifcellanea Curiofa. 
not oblig’d to accommodate his Scheme te 
Nature; for here he has made the Circle GF 
reprefenting the Earth very large in propor- 
tion to the Circle AD; and then indeed 
taking the point F in the Harth’s furface, 
and by lines from thence dividing the Angle 
AFD into what ever equal parts the inter- 
cepted Arches AB, BG, CD, fhall be un- 
equal. But if he had» confidered, that the — 
Earth is as it were a point in refpect of the 
Sphere of the fix’d Stars, nay the very annual 
Orbit of the Earth is almoft if not altogether 
imperceptible (faving the truth of Mr. Aook?s 
Attempt) he would have found that the Lines 
FB, FC, FD, mutt be allconceived as drawn 
from the point G, and then equal Angles © 
will intercept equal Arches, and equal Arches 
equal Angles: And fo it happens (at leaft 
beyond the poffibility of difcovery of fenfe) 
to the Eye onthe furface of the Earth. And 
befides he fhould have confidered , that all 
Obfervations Aftronomical are performed as 
from the Center of the Earth, and therefore 
it is that they keep fucha ftir about a Paral- 
lax; fo that his drawing his lines fo far from 
Gas F is, and to, another concentrick Circle 
fo nigh as AD, deceived him in this 
Point. | oe | 
The famous Gaffendus has written 4 large 
Epiftles on this Subject, the fubftance of all 
which is, that the Moon being nigh the Ho- 
vizon and looked at through a more foggy ~ 
Air, cafts a weaker Light, and confequently 
forces not the Eye fo much as when brighter; 
and therefore the Pupil does more inlarge it 
fclf, thereby tranfmitting a larger Projection - 
tis on 


TSS eevee a, el a ee 


Mifcellanea Curiofa. 269 
on the Retiza. In this Opinion I do find he 
is not alone, for in the Journals des Scavans 
this Difquifition being again revived by a 
French Abbe, he therein follows this Senti- 
ment of Gaffendus. It was firft publifhed in the 
3d Conference prefented to the Dauphin in 
August 1672. but by reafon of an Objection 
moved by Father Pardye, it was fain to be 
re-publifhed with fome additions and amend- 
ments in Oétob. 1672. The addition was, 
that this contracting-and enlarging of the 
Pupil caufeth a different fhape in the Eye; 
an open Pupil making the Cry/taline flatter 
and the Eye longer, and the narrower Pupil 
fhortning the Eye, and making the Cry/talline 
more convex, the firft attends our looking at 
Obje&ts which are remote or which we think 
fo; the latter accompanies the viewing Ob- 
jects nigh at end. Likewife an open Pupil 
and flat Cryftalline attends Obje&ts of a more 
fedate Light, whilft Obje&s of more forcible 
Rays require a greater Convexity and narrow 
Pupil. From thefe Pofitions the Abbe endea- 
-voured to give an account of our Phenomenon 
as follows. When the Moon is nigh the 
Horizon, by comparifon with interpofed Ob- 
jects, we are apt to imagine her much farther 
‘from us then when more elevated, and there- 
fore (fays he) we order our Eyes as for view- 
ing an Object farther from us ; that is, we 
fomethigg enlarge the Pupil, and. thereby 
_ make the Cryftalline more flat; moreover the 
duskifhnefs of the Moon in that pofture does 
not fo much ftrain the fight; and confe- 
quently the Pupil will be more large, and the 
‘Cryftalline more flat: Hence a larger Image 

fhali 


270 . Mifcellanea Curiofe. 
thall be projected on the Fund of the Eye, 
and therefore the Moon fhall appear larger. 
And this difpofition of the Eye that magnifies 
her, magnifies alfo the -divifions of our fore- 
mentioned Lattice, and confequently the by 
her Body fhall poflefs no more of the divifions 
than when fhe feems. lefs. Thefe two fore-— 
mentioned accidents, viz. the Moons ima- 
ginary diftance and duskifhnefs, gradually 
vanifhing as fhe rifes,a different Speczes'is here-: 
by introduced in the Eye, and confequently 
fhe feems gradually lefs and lefs, ’till again 
fhe approaches nigh the Horizon. Thefe two 
Opinions of Gaffendus and the Abbe being fo 
nigh a-kin , I fhall confider them both toge- 
ther, and firft I affert that a wider or nar- 
rower Aperture increafes not, neither dimi- 
nifhes the projection on the Retina. I know 
Honor atus Faber in his Syzopfts Optica endeavours 
to prove the clear contrary. to thismy Affer- 
tion, and that after this manner. Fig. 42. 
' AB isan Objet, E F the greater aperture 
of the Pupil, adniitting the projection KI 
on the Retina, whereas the lefler aperture - 
CD admits only the projection GH; but 
GH is lefs than KI, ,wherefore,a leffer aper- 
ture diminifhes the projection. 1. admire 
that any Man that. undertook (as Honoratus 
Faber) to write of Opticks more accurately 
than all that went before him, fhould. be 
guilty of fo very grofs.an Error; and,I. do 
more admire that the celebrated Gaffendus, 
-and with-him.the noble; Hevelius fhould be. of | 
the fame Opinion: For tho’ the *forefaid Fi- 
gure and Demontftration hold moft. certainly 
true in diredt proje@ions, as in_a.dark Room 
2 2 : ‘ with 


Maifcetanea Curtofa. 274 
with a plain’ hole; yet it will not hold in 
Projections made by RefraGtion, as it is in 
thofe on the Retiva in the Eye, by means of 
the Cry/tallime and other Coats and Humours 
of the Hye. Fora Demonftration of this ob- 
ferve Fig. 43. wherein let A B be a remote 
Object, and BF the Cryflalline at its large 
aperture, projecting the Image 1M_ on the. 
Retina. Let then CD be the lefler aperture 
of the Pupil before the Cry/ftaline : 1 fay the 
Image IM fhall be projected as large as be- 
fore, for the Cone of Rays EAF confifts 
_ partty of the Cone of Rays CAD, therefore 
where the former EAF is projected, the 
latter CAD, as being a part of the former, 
 fhall be projected alfo. So that no more is 
effected by this narrow Aperture , but that 
the fides of the radiating Cones are inter- 
cepted, .and confequently the Point I fhall be 
affected. with lefs light,, but it fhall. ftill be in 
the fame place: What is faid of that Cone 
and that Point may be faid of all other Cones 
and other Points of the Obje&. From:hence 
appears firft, the Invalidity of the Account 
given of. the Moons appearance by Gaffendus 
from this Reafon. 2dly, The Reafon ap- 
pears why a Telefcopes greater or lefler 
Aperture, makes no difference in the Angle 
it receives; for imagine EF to be an Objedct- 
glafs of a Telefcope, and ’tis plain. 3dly, 
’Tis. evident. why a greater or lefs Aperture 
on a.Telefcope fhonld make the Objects ap- 
pear Lighter or Darker, for thereby more or 
lefs Rays are admitted to determine on the 
Projection of each Point. But all this by the 
by. And this is fuficient fora Bearnenion. 
| | OQ 


« 


542 : Mifcellanea Caria 


of Gaffendus and Faber : But our forementioned 
Abbe fuperadds to a greater or leffer Aper- 
ture of the Pupil, as a neceflary Confequent, 
a greater and leffer Convexity of the Cry/tal- 
line, as alfo a lengthening and fhortening the 
Tube of the Eye. And this 1 muft confefs 
would do fomething if we find it truein our 
Cafe; and this let us try. Firft, fays he, 
the duskifhnefs of the Moon nigh ‘the Hori- 
zon admits the Pupil to enlarge it felf, the — 
Cryfrailine to flatten, and the Eye to lengthen. 
But what if we change our Objed, and in- 
ftead of the Moon take the diftance between 
fome of the fixt Stars; as fuppofe thofe of 
Orions Girdle) we fhall ‘ind the fame Pheno- 
menon in them, and yet I hope neither he nor © 
Gaffendus will aflert, that they at one time 
ftrain the Eye more than at another, or that 
at any time their fulgur ftrains the Eye at 
all; if he do, let him take Stars of the lefler 
Magnitudes , nay even thofe that can but 
juft be perceived, and then he will be tof 
vinced: Or let him confider whether this will 
hold in looking at the Sun through very dark 
Glaffes, which render the Sight thereof as 
inoffenfive to the Eye; as that of a green. 
“Field. But perhaps he will then fay that this 
other Reafon holds, which is 2dly, That the 
preater imaginary diftance at which we think 
the Moon near the Horizon, than when more © 
elevated, makes us Contemplate her as if 
really fhe was fo, viz. with ample Pupils, @c. 
but this I have fuficiently overthrown in my 
Remarks againft Des Cartes; therefore I pafs 
it over, only fubjoining that if there were 
any thing in this Surmife, my-thinks the A- 

rizontal 


Mifcellanea Curiofa. 272 
rizontal Moon fhould be fancied nigher to us 
than farther from us; for if we are for try- 
ing natural Thoughts; let us take Children 
to determine the Matttr, who are apt to 
think that could they go to the edge of that 
{pace that bounds their Sight , they fhould 
be able (as they call it) to touch the Sky ; 
and confequently the Moon feems then rather 
nigher to us than farther from us. 

After I had writ thus. far I accidentally caft 
my Eye upon Riccioli’s Treatife of Refraction, 
at the end of his 24. Volume of the Almageft, 
Lib. 10. Sett. 6. Cap.1. Queft. 13. wherin he 
fpeaks of our prefent Difficulty ; buf to my 
wonder I find him affert, that he and Father 
Grimaldi had often taken the Horizontal Sunand 
Moons Diameter by a Sextant, when to the 
naked Eye they appeared very large ; (Grimal- 
dus directing his Sight to the left edge, and 
Ricciolus to the right,) and that even by the 
Inftrument they always found the Diameters 
greater than when more elevated, the Sun 
often fubtending an Angle of almoft a De- 
gree, and frequently 45 Minutes, the Moon 
alfo 38 or 40 Minutes. This is downright 
contrary to the matter of Fa which I have 
before alledged, and diretly repugnant to 
the matter of Fad aflerted by the French. 
Abbe in the forecited Journal. Whether of 
tis be in the right I leave to accurate Ex- 
periment to determine, and fubmit the | 
whole to the decifion of the IMu/frious Roy- 
al Society. Only give me leave to add 
one word againft Riccioli, for had his Experi- 
ments been accurately profecuted, he fhould 

fig have 


274 Mifcellanea Curiofa. 
have tryed them when the Horizontal Moon 
- had look’d ten times more large in Diame- 
ter than ordinary; and then if it’ be true, 
that even by an Inftrument fhe will be found 
proportionally broader than really fhe fhould 
fubtend an Angle of 300 Minutes, or 5 De- 
grees: for very often I have feen the Moon 
when fhe appeared 10 times broader than or- 
dinary, which the fmall addition of 8 or to 
Minutes to. her ufual Diameter will never 
Caufe. } 
~ Laftly,as an Apology for my reviving this 
difquifition to that Noble Company of Exglifh 
Philofophers, I fhall only imitate the words 
of the forementioned Abbe’s Letter. Pour la 
Raifon de cette Apparence, & de la tromperie de 
nos Sens, je la tiens plus Difficile a trouver, que 
les plus grands Equations d Algebre, & quand 
vous y aurex bien penfe, vous m’ Obligerez de m 
en dire voftre Sentement, &c. PS ode 
After which | have only to fubfcribe my 
felf-an unworthy Member, and an humble 
Servant and Admirer of that Iluftrious Com- 
pany. : 


machi. 83, William Molyneux. 


The 


M. ifcelanea Curiofa. 2 7 5 


The Sentiments of the Reverend 
and Learned Dr. John Wallis 
_R. S. Soc. upon the aforefaid 

Appearance, communicated in a 


Letter to the Publifber. 


A S to the laft Inquiry (concerning which, 
you fay, the Royal Society would be 
glad to know my Opinion ;) about the appa- 
rent Magnitude of the Sun near the Horizoz, 
greater than when confiderably high : 

The Inquiryis Ancient : And, I remember, 
I difcourfed it near forty Years ago with 
Mr. Foffer, then Profeffor of Aftronomy in 
Grefham College. Who did then affure me 
(from his own Obfervation, I fuppofe, for 
I have never examined it my felf,) that the 
apparent Magnitude taken by Inftrument 
(however the Fancy may apprehend it) is not 
greater at the Horizon, than when higher. 
And Mr. Cafwel (when your Letter was com- 
municated to our company here) affirmed the 
fame. _ oes | 

And (though I have not my felf made the 
Obfervation) I do not doubt but the thing is 
fo. For it is agreed, That Refraction near 
the Horizon, though (as to appearance) it 
alter the Altitude of the thing feen ; yet it 
alters not the Azimuth at all. ) 


se And 


276 Mifcellanea Curiofa. 

And it muft needs be fo. For, fince this 
equally refpects all points of the Horizon 5 let 
the Refraction be what it will, the whole Ho- 
rizon can be but a Circle: So that there is — 
no room for the breadth of a thing (as to 
the Angle at the Eye) to be made greater, 
whatever its Tallnefs may (the Refraction 
not equally affecting all parts in the Circles 
‘of Altitude.) Nor is there any reafon why 
this fhould rather thruft the other, than that 
the other thruft this, out of place. , : 

Whereas, in the Altitude, it is otherwife : 
For while what is near the Horizon is inlarg- 
ed, that which is further off is thereby con- 
~ traé&ted: which as to the Azimuth or Horizon- 
‘tal Pofition cannot be. — 

In Speétacles indeed it is otherwife ; for 
they reprefent the Object every way enlarg- 
ed; and do thereby hide the adjacent parts. 
But in Refraction by Vapours, fuppofing all 
parts of the Horizon equally affected by them, 
one part cannot be expanded in breadth 
(whatever it may be as to the heighth) with- 
out thrufting out another (for the whole 
Horizon can be but a Circle) and, why one 
part rather than another ? Peis 

Unlefs we would fay (as perhaps we may, 
if there fhall appear a neceflity for it) That 
the Rays of a lucid Body do expand them- 
felves every way to the prejudice of the parts 
adjacent, by covering them. weet 

But fuppofing (which I am apt to believe, 
till the contrary fhall be evinced by Experi- 
ment) that the Sun or Moon’s apparent Dia- 
meter taken by Inftrument near the Horizon, 
is the fame as taken in a higher Pofition, (I 

: 3 mean 


Mifcelanea Curiofa. 279 
mean its Horizontal Diameter, or that paral- 
Jel to the Horizon ; forthe erect Diameter, in 
a Circle Perpendicular to the Horizon, may by 
the Refraction be varied, and thereby made, 
not greater, but lefs than when higher; as 
hath been noted in the Name of Sol Elkpticus 
at the Horizon.) Suppofing, I fay, that 
the Sun’s apparent Diameter Horizontal, ta- 
ken by Inftrument, is the fame near the Ho- 
rizon, asin a higher Pofition, I take its Ima- 
ginary greatnefs which is fanfied near Horizon, 
to be only a deception of the Eye ; or rather 
the Imagination from the Eye. : 

For fure it is, that the Imagination doth 
not eftimate the greatnefs of the Objed feen, 
only by the Angle which it makes at the Eye; 
but, by this compared with the fuppofed di- 
ftance. | 

True it is that, Ceteris paribus, we judge 
that to be the greater Obje&t, which makes 
at the Eye the greater Angle: But not fo if 
apprehended at different Diftances. 

For if through a Cafement (or lefler aper- 
ture) we fee a Houfe at 1oc Yards diftance 3; 
this Houfe (though feen under a lefs Angel) 
doth not to us feem lefs than the Cafement 
through which we fee it, (or this greater than - 
that, becaufe it makes at the Bye the greater 
Angle:) But the Imagination makes a com- 
parative Eftimate from the Angle and Di- 
{tance jointly confidered. : 

_ So that, if two things feen under the fame 

or equal Angles, if to one of them there be 

ought which gives the apprehenfion of a 

greater Diftance, that to the Imagination will 

appear greater. | 

bios Fi3 2 Now 


278 Mifcellanea Curiofa. 

Now fure it is,that one great advantage for 
Eftimating of a ‘thing feen, is, from the va- 
riety of intermediate Objects between the 
_ Eye and the thing feen. For then the Ima- 
gination muft allow room for all thefe 
things. 

Hence it is that if we fee a thing over two 
Hills, between which there lies a great Valley 
unfeen, it will appear much nearer than if 
we fee the Valley alfo: And it will appear as 
juft beyond the firft Hill. And if we move 
forward to the top of the neareft Hill (that 
fo the Valley may be feen) it will then appear 
much further than before it did. — 

And on this account it is, that the Sun 
fetting, appears to us as if it were but juft 
beyond the utmoft of our vifible Horizon ; -be- 
caufe all between that and the Sun is not 
feen. And,upon the fameaccount, the Hea- 
ven it felf (ceineiConmgataE ty the vifible 
fTorizon. 

Now when the Sun or Moon is, near the 
Horizon, there isa profpe& of Hills, and Val- 
lies and Plains and Woods, and.Rivers; and 
variety | of Fields, and Inclofures, between 
it.and us’: which prefent to our Imagination 
a great Diftance capable of) receiving all 
thefe:» Or,:if it fo chance that (in fome Po- 
fition) thefe Intermediates are not adually. 
féen :: Yet having beemaccuftomedto fee them, 
the Memory fuggelts to:us a view as large, as 
is the-vifible ddorix0n. | 

' Bat/!wiren® the Sum or; Moon j isin a higher 
Pofition; we fee nothing between us andthem 
<unlefs perhaps fome Clouds), and:therefore 
nothing to prefent to our Imagination fo, gt eat 
ve Diftance as the other j Be “And 


a Mifcelanea Currofa. 279 
_ And therefore, though both be feen under 
the fame Angle, they do not appear (to the 
Imagination) of the fame bignefs, becaufe 
~ not both fanfied at the fame Diftances: But 
that near the Horizon is judged bigger (be- 
caufe fuppofed farther off) than the fame 
when ata greater Altitude. 

?Tis true, that as to fmall and middling 
_Diftances (befides this Eftimate from Inter- 
mediates) the Eye hath a means within it felf 
to make fome Eftimate of the Diftance. As, 
when we already know the bignefs of a thing 
feen, to which we have been accuftomed ; as 
a Man, a Tree, a Houfe or the like: If fuch' 
thing appear to us under a fmall Angle, and 
-indifting, and faintly coloured; the Imagi- 
nation doth allow fuch Diftance, as to make 
fuch a thing fo to appear. And, if this, thro’ 
a Profpective Glafs, be repefented to us un- 
der a bigger Angle, and more diftiné: It is 
accordingly apprehended as fo much nearer. - 

But the cafe is otherwife, when we do not 

by the known bignefs, judge the Diftance; 
but, by the fuppofed Diftance, judge of the 
bignefs ; asin the Cafe before us. A 

_ And accordingly, different Perfons, accord- 
ing to. different fancied Diftances, judge ve- 
ry differently. As, if two Stars be fhewed 
to ignorant Perfons, and you ask how far they 
feem to be afunder: one perhaps will fay a 
Foot; another. a Yard, or more: And one 
fhall fay, the Sun appears to him as big as a 
_Bufhel ; another, as big as a Holland Cheele : 
pe eitimating according to the fancied Di- 
‘ftance. beat v 


T ‘4 c. Again 


280 Mifcellanea Curiofa. 
Again ; in our two Eyes (when the Object © 
is feen by both) there is yet. another means — 
of eftimating how far off it is. (And'it is | 
this by which we judge of Diftances.) Name- — 
ly, there are, from the fame Obje&, two dif- 
ferent vifual Cones, terminated at the two 
Eyes: Whofe two Axes contain, at the Ob- © 
jet, different Angles, according to different 
Diftances: An accuter Angle at a great — 
Diftance, and more obtufe when nearer. 
Now, that fuch Obje& may be feen by both 
Eyes, clearly; it is requifite that the Eyes be 
put into fuch a Pofition, as that the Sight of 
_ each Eye receive the refpective Axe at right 
Angles. Which requires a different Pofition 
of the two Eyes, according to the different 
Diftance of the Objet. | a 
As will manifeftly appear ; ifwe look, with 
attention, on a Finger (or other fmall Ob- 
ject) at two or three Inches diftance from the 
Kye; and then upon another like Obje& at 
three or four ¥ards beyond it: (and this al- 
ternately feveral times. For *twill be mani- © 
feft, that while we look intently on the one, © 
we do not fee the other (or but confufedly} 
though both be juft before us. And, as we — 
change our view, from the one to the other, | 
we manifeftly feel a Motion of the Eyes (by 
sab Mufcles) from one pofture to ano- 
hon BR to gi wh vag hs 2 | 
And according to the different pofture in — 
the Eyes, requifite to a clear Vifion by both, 
we eftimate the Diftance of the Object from — 


pS: | a 

ve And hence it is,that they who have loft the 

_ Bight of one Eye, are at a great difadyantage, 
ay 5 Filia \ Pe iy MT RR rae as 


Mifcellanea Curtofa. 28: 
as to eftimating Diftances, from what they 
could do while they had the ufeof both. _ 
But now when the Diftance grows {o great, 
as that the Pofition of thefe vifual Axes be- 
come Parallel, or fo near to Parallel, as not 
to be diftinguifhable from it: This advan- 
- tage is loft, and we can thenceforth only 
conclude, that it is far off; but not how far. 
Hence it is, that our view can make no 
- diftin@tion of the Moon’s Diftance, from that 
of the other Planets, or even of the fixed 
Stars: But they feem to us as equally remote 
from us ; though we otherwife know their 
-Diftances from us to be vaftly different. Be- 
caufe the Parallax (as I may fo call it) from 
the different Pofition of the two Eyes, isquite 
loft, and undifcernable, in Diftances much 
lefS than the leaft of thefe. 
_ And fo, of the fixed Stars among them- 
felves : Which, though they feem equally re- 
mote from us; many (for ought we know) 
be at Diftances vaftly different. Nor can we 
tell, which of them isneareft: (unlefs perhaps 
we may reafonably guefs, thofe to be neareft, 
which feem biggeft.) Becaufe, here not on- 
ly the Parallax from the Diftance of the two 
Eyes 3 and that from the Earths Semidiame- 
ter ; but even that from the Semidiameter of 
the Earths great Orb, is quite loft ; and none 
remaining, whereby to eftimate their Diftance 
from us. i | | 
_ But (to return to our cafe in hand ;) tho’ 
as to fmall Diftances, we may make fome 
eftimate from the known Magnitude of the 
Obje& : And, as to middling diftances, from 
the Parallax (as I may call it) arifing from 
Pi the 


282 Muifcellanea Curiofa. 


the interval of the two Eyes; Yet even this 
latter will hardly reach beyond, if fo far as 
the vifible Horizon: and all beyond it, is loft. 
So that, there being nothing left to affift 
the fancy in eftimating fo great a diftance, 
‘but only the- intermediate Objects : Where 
thefe intermediates appear to the Eye, (as, 
when the Sun or Moon are near the Horizoz -) 
the diftance is fancied greater, than where 
they appear not, (as when farther from it :), 
and confequently (though both: under the 
fame or equal Angles) that near the Horizon 
is fancied the greater. And this I judge to 
be the true reafon of that appearance. 
You will excufe ([hope) what excurfion I 
have made; becaufe though fome of them 
might have been fpared, as to the prefent 
- eafe; yet they are not impertinent to the bu- 
finefs of Vifion ; and the eftimate to be thence — 
made, of JAdagnitudes and Diftances, by the 
Imagination. | | at Ae 


The Sun’s Eclipfe Aéay 1/f. was here ob- 
ferved about 4 a Digit ; between one and two 
a Clock after noon. be 


~ Mifcellanea Curiofa. : 282 


A Demonfiration of an Error com- 
mitted by common Surveyors in 
comparing of Surveys taken at 
long Intervals of Time arifing 
from the Variation of the Mag- 
netick Needle, dy William Mo- 
lyneux. E/; “Eb BSe oa 


HE Variation of the Magnetick Needle 

is fo commonly known, that I need not 
infil much on the Explication thereof; ’tis 
certain that the true Solar Meridian, and the 
Meridian fhewn by an Needle, agree but in 
a very few places of the World; and this too, 
but for a little time (if a moment) together. 
The Difference between the true Meridian 
and Magnetick Meridian perpetually vary- 
ing and changing in all Places and at all 
Times; fometimes to the Eaftward, and 
fometimes tothe Weftward. 

On which account ’tis impoffible to com- 
pare two Surveys of the fame place, taken at 
diftant times, by, Magnetick Iniftruments, 
(fach as the Circumferentor, by which. the 
Down Survey, or Sir William Petty’ s. Survey .of 
Ireland was taken) without due allowance be 
made for this Variation. To which purpofe 
we ought to know the Difference between. 
the Magnetick Meridian and true Meridian 

at 


284 Mifcellanea Curiofa. 
at that time of the Dowz Survey, and the 
faid difference at the time when we make a 
new Survey to compare with the Dowz 
Survey. _ 

But here I would not be underftood as if 
I propofed hereby to fhew, that a Map of 
the fame place, taken by Magnetick Inftru- 
ments at never fo diftant times, fhould not at 
one time give the fame Figure and Comtents as _ 
at another time. This certainly it will do 
moft exactly, the variation of the Needle 
having nothing to do either in the Shape or 
Contents of the Survey. All that is affected 
thereby, is, the Bearings of the Lines run by 
the Chatn, and the Boundaries between 
Neighbours. And how this may caufe a con- 
fiderable Error (Cunlefs due allowance be ~ 
made for it) is what I fhall prove moft 
fully. 

In order to which, let us fuppofe that about. 
the Year 1657. (at which time the Dowz 
Survey was taken) the Magnetick Meridian 
and true Meridian did agree at Dubliz, or 
pretty nigh all over Jreland ; that is to fay, 
that there was no Variation. And indeed 
by Experiment it was at that time found, as 
I am well aflur’d, that at Dublin it was hardly 
half a Degree. | 

Let us fuppofe that in the year, 1695. the 
Variation was 7 Degrees from the North to 
the Weftward ; that it was really fo, I be- 
lieve Iam pretty well aflured , from an Ex- 
periment thereof made by my ielf with all 
diligence. But this is not material, let us © 
now only fuppofe it. HAL aed 


Let 


Mifcellanea Curiofa. 285 


Let AB reprefent the Survey of two 
Town-Lands, one in the pofleflion of 4, and. 
vother in the pofleflion of B, which we call 
A Town-Land and B Town-Land, taken by 
the Down-Survey , Anno 1657. when there 
was no Variation. 

Let the Line NS running through the 
Point P be the true Meridian, and confe- 
quently the Magnetick Meridian alfo at that 
time, becaufe of the fuppofed no Variation, 
and let this Line NS be alfo the Boundary 
between the two Town-Lands 4 and B. 

In the year 1695. when the Variation ‘is 
7 Degrees from the North to the Weftward, 
B having a Map of the Down Survey, and be- 

- ing fufpicious that his Neighbour -4 had in- 
croached on him by a Ditch PQ, imploys a 
Surveyor to inquire into the matter: The 
Surveyor finds by his 4¢@ap that the Boundary 
between B and his Neighbour 4 run from the 
Point P through a Meadow dire@ly according 
to the Magnetick Meridian SPN; but ob- 
ferving the Ditch P © caft up much to the 
Eaftward of the prefent Magnetick Meri- 
dian, he concludes that 4 has incroached on 
B, and that the Ditch ought to have been 
caft upalongft the Line Pq, the Angle Q Pq 
being an Angle of 7 Degrees , that is is the 
piclent Variation of the Needle; and the 

ine Pq the prefent Magnetick Meridian: 
For which Variation , not making any al- 
lowance, he pofitively determines that B has 
all the Land in the Triangle Q P 4, more 
than he ought to have; and that his Ditch 
ought to run alongtt the Line P q. 


Bas 


286 © Mifcellanea Curiofa. 


’Tis true indeed, if the Surveyor go the 
whole furround of the Lands Aand B, he 
will find their Figure and Contents exactly 
agreeable to the Map here exprefled. But 
then the Bearings of the Lines are all 7 De- 
grees different from the Bearings in the Map, 
and they will run in and out upon the adja- 

cent Neighbouring Lands, and caufe endlefs 
Differences between their Poffeffors; as is 
manifeft from the Figure: wherein the prickt _ 
Lines reprefent the Difagreement in the 
Bearings of the Lines, protracted from the 
Point P'; and we fee A incroaching on his 
Neighbours on the Weftward, as he incroaches 
on 8B, and Bs EHaftward "Neighbours in- 
croaching on him, and fo forward and clear 
round. Whereas, by a due allowance for the 
Variation of the Needle, all this Confufion 
and Difagreement is avoided, and every 
thing hits right. 

Thus for inftance in the Cafe before us, 
knowing that the Magnetick Variation has 
caufed the prefent Magnetick Meridian to 
fallin the Line z g P s, 7 Degrees from the - 
‘North to the \Weftward ; ; to reduce this to 
the Magnetick Meridian at the time of the 
Down Survey, I muft make the Meridian of 
my Map to fall 7 Degrees to the Eaftward of 
my Magnetick Meridian ; as we fee the Line 
PQ falls 7 Degrees to the Eaftward of the 
Line P q: 

What is here faid on fuppofition that the 
Magnet had no Variation at the time of the 
firft Survey taken, and that it had 7 De- 
grees variation Weftward:at the time of the 
fecond Survey, may ealily He accommodated 

Ta 


Mifcelunea Curiofa. 287 
to the fuppofal of any other Variations at 
the firft and fecond Surveys, Afutatis mue 
tandw, for knowing the Variations we know 
_ their Difference; and if we know their Dif- 
ference, this gives us the Angle O. Pq, by 
which we reduce them to each other. 

The beft way therefore to make Maps in- 
variable, conftant and everlafting , were for 
the Surveyors , who ufe Megnetick Inftru- 
ments to make always allowance for the 
Magnetick Variation, and to protraé& and 
lay dew their Plats by the true Meridian. 
This a wary Sailer is fully convinced of : 
and therefore in Steering his Courfe, he con- 
{tantly allows for the prefent Variation, which 
he obferves by the Azuuth Compafs, or elfe 
he would mifs his appointed Harbour oftner 
then he would hit it: For ‘ two Points on 
the Globe keep the fame Bearing to each 
other by the Magnetick Meryidian for any 
time together: And though, the Variation 
be flow, yet in a long Courfe, or in times 
pretty diftant, 1t may caufe vaft Errors, un- 
lefs allowed for. Thus for inftance, fup- 
pofe in the year 1660. a Sailor had fteered 
from the Land’s end of Exgland to Cape Fini- 
‘fter in Spain, by his Magnetick Compafs 
a direct South Courfe; and that at thattime ~ 
there were no Variation. Afterwards Azzo 
1700. when there was (fuppofe) 7 Degrees 
of Variation from the North to the Weft- 
ward, another Sailor intending to make the 
fame Paflage, fteers diretly the fame South- 
erly Courfe by his Magnetick Compafs: I fay, . 
this laft Seaman will be carried far into the 
Bay of Bifcay to the Haftward, and will ier 
| 5 


\ 


288 Mifcellanea Curiofa. 
of his defired Port by many Leagues ; but if 


in his Courfe he hath allowed for this Varia- 


tion, and inftead of failing a direé Southerly 
Courfe by his Compafs, he had fteer’d 7 De- 
grees from the South to the Weftward, he 
had hit his Point. Whether thefe be the true 
Bearings of thefe two Places, it matters not : 
_ We go onto the Suppofition that they are. 
Perhaps it may be objected, That Surveys 
may be taken withoutMagnetick Inftruments, 
and that therefore this Error arifing from the 
Megnetick Variation, and Change of the 
Bearings of Lines, may be avoided. To 


which I anfwer, firft, That granting a Sur- > 


vey may be taken without Magnetick Inftru- 
ments, this is nothing againft what we have 
laid down relating to Surveys that are taken 
with Magnetick Inftruments, as the Down 
Survey actually was, and moft Surveys at pre- 
fent aétually are taken therewith. Secondly, 
Though a Survey may be taken truly with- 
out Megnetick Inftruments, fo as to fhew the 
exact Angles and Lines of the Plat, and con- 
fequently the true Contents, yet this will 
not give the true Bearings of the Lines, or 
fhew my Pofition in relation to my Neigh- 
bours, or the other parts of the Country. | 
This muft be fupply’d by the Magnet, or, 
fomething equivalent thereto, as finding a 
true Meridian Line on your Land by Celeftial 
Obfervations. And I doubt not but the an- 
cient Egyptians, before the difcovery of the 
_ Magnet were forced to fome fuch Expedient 
in their Surveys and Applotments of Lands 
between Neighbour and Neighbour, after 
the Inundations of the Nile, which, we are 
| - told 


Muifcelianea Curiofa. 289 
told, gave the firft Original to Geometry 
and Surveying. Abfolute Neceflity and Ufe 
having introduced thefe, as Delight and Di- 
verfion introduced Aftronomy amongft the 
Chaldeans. | 
- And this brings me to another Objection 
which may be made againft the Inftance be- 
fore laid down: It may be faid, That cer- | 
tainly the Surveyor which B imployed was 
very ignorant, who would choofe to judge 
of the Line P QO, rather by its bearing than 
by determining the. Point QO, by meafuring 
from AH and G. Tothis I anfwer, What if 
both the Points HandG were vanifh’d fincethe 
Down Survey was taken ? What if the whole 
face of the Country were chang’d, fave only 
the Point P? and the Line P O? How fhall 
the Surveyor then judge of the Line P O but 
by its bearing ? That this is no extrava- 
gant Suppofition, we have an Example in 
Egypt above-mentioned, where the Nile lays 
all flat before it, and fo uniformly covers all 
with Mud, that there is no diftincion. In 
fuch a Cafe your bearing muft certainly help: 
you out, there is no other way. | 

But I anfwer fecondly, To fay that the 
Surveyor might have determin’d the Point Q 
by admeafurement from G and #, or any 
other adjoining noted Points, as from F, kK, /, 
&e. tis very true; But then ’tis again{t our 
Suppofition. Iam upon fhewing an Error 
that arifes from judging of the Line P O by 
Magnetick, bearing, and to tell me that this 
‘might be avoided by another way, is to fay 
nothing. I my felf oe it may be hae | 

. e 


290° «Mifcellanea Curiofa. _ 
ed by allowing for the Variation; but ftill it 
is an Error, till it be avoided. NC 
But thirdly, if B’s Surveyor do not allow 
for the Variation of the Needle, he will ne- 
ver exactly determin even the Points G, F, 
H, K, &c. orany other Points in the Plat; 
but inftead thereof will fall on the Points g, /, 


” From what has been laid down, we may 
fee the abfolute neceflity of allowing for the 
Variation of the Magnet, in comparing old 
Surveys with new ones; for want of which 
great Difputes may arife between neighbour- 
ing Proprietors of Lands: and it were to be 
wifh’d that our Honourable and Learned 
_ . Judges would take this Matter into their 
Confideration whenever any Bufinefs of this 
kind comes before them. Hitherto an abfo- 
lute Acquiefcence in the Down Survey, with- 
out any of the fore-mention’d Allowance, has 
been agreed upon as a ftanding Rule in our 
Courts of Judicature in Ireland, but that ma- 
ny Men may be injured thereby, I fuppofe 
is manifeft from what foregoes. fom THE 

I have only this to add, That leaft I be 
thought herein to ftrike at the Truth or Ex- 
actnefs of the Down Survey, ’tis not at all 
the intention of this Paper, but rather to 
confirm it, by fhewing which way Men 
ought to Examine it truly, and not by the 
common ways ufed by them, which rather 
confound it, and all that claim under it. | 


See the Table Fig. 44. 


Mifcellanea Curiofa. 29% 
Although this Paper was chiefly defigned 
for the ending of Contefts in the Kingdom of 
4reland about the interefts of fome of thofe 
whofe Lands are Neighbouring, and have 
been furveyed by Magnetick Inftruments, 
yet confidering its univerfal Ufe, it was 
thought it would be very grateful to the Cu- 
tious to publifh it here. : 


292  Maifcellanea Curiofa. 


A Propofal concerning the Parallass 
of the fixed Stars, m Reference 
- tothe Earths Annual Orb. In” 
feveral Letters of May the 2d. 
June 29. and July 20.1693. from 
Dr. John Wallis to William 
Molineux Ef; 73 | 


Sig. : 
| Am obliged to you for two Books which 
you have been pleafed to fend me, that 

of your Sciothericum Telefcopicum, and that of 
Dioptricks;, which you have performed fo well, 
that Ihave not been better fatisfied with any 
that I have feen of that Subje@. J fhould not 
fo long have neglected to return my Thanks 
for them, but that I thought a Letter of bare, 
Thanks to be too empty, unlefs I had fome- 
what elfe to fend with it. - oo 
You will, 1 hope, give me leave (though I 
have not the opportunity of being perfonally 
known to you) to fuggeft a Speculation, which 
hath beenin my Thoughts thefe Forty Years 
or more ; but I have not had the opportu- 
nity of reducing it to Practice, as being not 
fo well ftored with neceflary Inftruments of 
that kind, nor much exercifed to Telefcopick 
Obfervations. And though I have many 
Years fince fuggefted it to others, yet nel- 
Bee ther 


— Mifcellanea Curifa. 293 
ther have they had leifure of convenience of 
putting it in Practice. : : : 

It is concerning the Parallax of the fixed 
Stars, as tothe Earths Annual Orb. | 

Galileo complains of it a great while fince 
Cin his Syffema Cofmicum) as a thing not at- 
tempted to be obferved with fuch diligence 
as he could wifh, and I doubt we have the 
fame caufe of. complaining ftill. I know that 
Dr. Hook and Mr. Flamftead have attempted 
fomewhat that way, but have defifted before 
they came to.any thing of Certainty. What 
hath been done to that purpofe abroad I 
know not. | | 

Galileo hath fuggefted divers things confi- 
derableinordertoit. — 7 

As to the times of. Obfervation ; That it 
fhould be when the Sun or Earth are in the 
Tropicks, or as near thereto as may be: Be- 
caufe at thofe times, if any, will be the 
greateft difference obfervable in their meri- 
dional Altitude. : 

As to the Stars to be obferved, That they 
fhould be fuch as are as near as may be to 
the Pole of the Ecliptick: For fuch as are in 
the. Plain of the Ecliptick, or near unto it, 
though they may be fometime nearer, fome- 
time farther from us, (which might fome- 
what alter their apparent Magnitude, if it 
were fo, much as to be obfervable) yet it 
would little or nothing alter the Parallac- 
tick Angle, as Galilelo doth there demon- 
iteate.. 

He notes alfo, that in a bufinefs fo nice, ° 
the ordinary Inftruments of Obfervation 
(though pretty ee would be infafficient 


vt 
3 (ne 


294 Maifcellanea Curiofa. 
(he doubts) for this purpofe, and doth pro- 
pofe, that by the fide of fome Edifice or Moun- 
tain, at fome Miles diftance, the fetting of 
fome noted Star (as that of Lucida Lyre) 
might be obferved at thofe different times of 
the Year, which might be equivalent to an 
Inftrument whofe Radius were fo large. 
_ Which were a good Expedient if Practica- 
ble; but I doubt the Denfity of our Atmo- 
fphere is fo great, as that it will be hard to 
difcern a Star juft at the Horizon, or even 
within fome few Degrees of it: And that the 
Refraction would be there fo great, and fo 
uncertain, as not to comply with fo curious 
an Obfervation. | Ap nH 
That which occurred to my Thoughts upon 
thefe Confiderations, was to this purpofe ; 
That fome Circumpolar Stars (nearer to the 
Pole of the Equator than is your Zenith, and 
not far from the Pole of the Zodiack) fhould 
be made choice of for this purpofe. And in 
cafe the Meridinal Altitude be difcernably 
different at different times, fo will alfo-be 
their utmoft Eaft and Weft Azimuth, which 
may be better obferved than their Rifing or 
Setting: And this will be not obnoxious to 
the Refra&ion, as is the Meridional Alti- 
tude ; (for though the Refraction do affect the 
Altitude, yet net the Azimuth at all); and 
we may here have choice of Stars for the pur- 
pofe; which in Obfervations from the bot- 
tom of a Well we cannot have; being there 
confined to thofe only which pafs very near 
our Zenith, though very fimall Stars. 


Maifcelanea Curiofa. 295 

I would then take it for granted, as a thing 
_ at leaft very probable, that the fixed Stars 

are not at all (as was wont to be fuppofed) at 
_ the fame diftance from us; but the diftance 
of fome, vaftly greater than of others; and 
confequently, though as to the more remote, 
the Parallax may be undifcernable; it may 
‘perhaps be difcernable in thofe that are near- 
er to us. 

And thofe we may reafonably guefs (tho’ 
We are not fure of it) to be neareft to us, 
- which to us do appear biggeft and brighteft, 
as are thofe of the Firft and Second Magni- 
tude; and there are at leaft of the Second 
Magnitude, pretty many not far from: the 
Pole of the Ecliptick, (as that in particular, 
in the Shoulder of the lefler Bear): And in 
-cafe we fail in one, we may try again and a- | 
gain on fome other, which may chance to 
_-be nearer to us than what we try firft. And 
Stars of this bignefs may be difcerned by a 
moderate Telefcope, even in the day-time; 
efpecially when we know juft where to look 
for them. 

The manner of Obfervation I conceive, 
may be thus: Having firft pitched upon the 
‘Star we mean to obferve, and having then 
sconfidered (which is not hard to do) where 
-fuch Star is'to be feen in its greateft Eaft or - 
Welt Azimuth ; it may be then convenient 
to fix! very firm-and fteadily on fome Tower, 
‘Steeple, or other high Edifice (in a convent- 
-ent fituation) a good Telefcopick Objedt-glafs 
in fuch pofition, as,may be proper for view- 
ing that Star. And-at a due diftance from it 
near the Ground, build on purpofe (if alrea- 

U 4 dy 


296 Mifcellanea Curiofa.. 

dy there be not any) fome little Stone Wall, 
or like Place, on which to fix the Bye-glafs, 
fo as to anfwer that Object-glafs: And ha- 
ving fo adjufted’ it, as through both to fee 
that Star initsdefired Station, (which may beft 
be done while the Star is to be feen by Night 
in fich fituation, near the time of one of the 
Solftices), let it be there fixed fo firmly, as 
not to be difturbed, (and the place fo fe- 
cured, as that none come to diforder it), 
and care be taken fo to defend both the 
Glaffes, as not to be endangered by Wind 
and Weather. In which contrivance I am 
beholden to Mr. Yohu Cafwel M. A. of Hart- 
ball in Oxford, for his Advice and Affift- 
ance ; with whom Lhave many Years fince, 
communicated the whole matter. — 

This Glafs being once fixed (and a Mi- 
crometer fitted to it, fo as to have its Threds 
perpendicular to the Horizon, to avoid a- 
ny inconvenience which might arife from 
diverfity of Refra@ion if any be) the Star 
may ‘then be viewed from time to time (for 
the following Year or longer) to fee if any 
change of Azimuth can be’ obferved. 

This I thought fit to recommend to your 
Confideration, who’ do fo well underftand 
Telefcopes, and the managery of them ; not 
knowing any who is more likely to’ reduce 
it to Pra@tice. Ff you fhall: think fit to give 
your felf the trouble of attempting the Ex- 
periment, and ‘that it fucceed well, it’ will 
be a noble Obfervation, » ‘and worth ‘the ‘La- 
bour : And, if it fhould‘mifcarry; ‘the “imei: 
| Hope would not be ef Pade 

” “fut 


 Mifcellanen Curtofa. 3 297 


But when I fuggeft (asa convenient Star 


‘for this purpofe) the fhoulder of the lefler 
’ Bear (as being the neareft to the Pole of the 
Zodiack of any Star that is of the firft or 
fecond Magnitude), I do not confine you to 
that Star; but (without retracting that) 
fuggeft another ; namely, the middle Star, 
in the Tail of the great Bear, which (tho’ 
-‘fomewhat farther from the Pole of the Zo- 
diack) isa brighter Star than the other, and 
may be nearer to us. , 

But I do it principally upon this Confider- 
ation : namely, That there is adhering to it 
a very fmall Star, (which the Arabs call 
Alcor, of which they have a Proverbial fay- 
ing, when they would defcribe a fharp-fight- 
‘ed Man; That he can difcern the Rider 
on the middle Horfe of the Wayn, and of 
one who pretends to fee fimall things but o- 
ver-look much: greater , Vidit Alcor at non 
 Lunam plenam): Which Hevelius in his Ob- 
fervations, finds’to be diftant from it.about 
- 9 Minutes, and 5 or 10 Seconds: Sothat - 
befides the advantage of difcovering the Pa- 
rallax of the greater Star, if difcernable. 
‘Their difference of Parallax of that and 
of the lefler Star“(being both within the 
reachiof a Micrometer) may do our Work . 
as well. For if that of the greater Star be 
difcernable, but that of the leffer be either 
motidifeernable; or Jefs difcernable.. Their 
different idiftances ‘from each other at dif- 
ferent times of the the Year, may, perhaps 
(without farther: Apparatas) be difcerned by 
‘a good»Telefcope of a competent length, 
| tur nifhed with a Micrometer, if carefully 
: Fhe pre- 


998) = =Mazfcellanea Curiofa. 
_preferved from being difordered in the Inter- 
vals of the Obfervations; and difcover at 
once, both, that there 1s a Parallax, and 
that the fixed Stars are at different diftan- 
ces from us, wherein, that I be not mifta- 
ken, my meaning is not, that the Inftrument — 
or Micrometer fhould be removed for the 
obferving of the lefler Star; but that (when 
the Azimuth of the greater Star is taken) 
by a Micrometer (confifting of divers fine 
Threads parallel and tranfverfe) may -(at the 
fame time) be obferved the Diftance of the — 
two Stars, each from other, in that Pofiti- 
on (both being at once within the reach of 
the Micrometer ;) which diftance (the In- 
ftrument remaining unmoved) if it be found 
(at different times of the Year) not to be 
the fame ; this will prove, that there is a — 
diflerent Parallax of thefe two Stars. me 
This latter part of the Obfervation (of 
their different diftances at different times) 
J fuggeft, as more eafily practicable though 
not fo nice asthe former. For it may bedone 
I think, without any further pparatas there 
than a good Telefcope, of ordinary form, 
farnifhed with a Micrometer, (this being 
carefully kept unvaried’ during the Interval 
of thefe Obfervations.. And if this part only 
of the Obfervation (without the other) be 
urfued 3 it matters not though the two Ob- 
Fopineiiag (near the two Solftices) be, one at 
the Haftern, the other at the Weftern Azi- 
muth (whereby both may be taken in the . 
Night-time,) for the diftance muft (at both — 
Azimuths) be the fame, if after obferving 
the Azimuth of the greater Star it be me | 
é CEie 


Mifcellanea Curiofa. 299 
 ceflary to move the Micrometer for meafur- 
ing its diftance from Alcor that may be done 
another Night (and it is not neceflary to be 
done atone Obfervation) for that diftance, 
and cannot be difcernably varied in a Night. 
or two. aS ify 

I fhall give you no farther trouble at pre- 
fent, but fubfcribe my felf, Sir, 


Yours, &c. 


A 


300 Mifcelanen Curiofa. — 


A Difcourfe on this PROBLEM; 


Why Bodies diffolved in Menfirua 
Specifically lighter than them-— 
felves, frou therems ~~ 


By Mr. WiLLiaM MotyNeux, of 
Dublin, Member of the Royal Soczety, — 


“FA4HE Liberty of Philofophifing being 
now univerfally granted between all 
Men, I am fure that a difference in Opinion 
will be no breach of affeGtion between two in- 
tirely Loving Brothers: And therefore I fhall — 
take the freedom’to propofe my own Thoughts 
in a matter wherein my Brother Mr. The- 
mas Molyneux hath appeared publickly in the 
Novelles de la Republique des Letres, Mois @ 
Aout 1684. Art 4: and Afou de Fanvier 1685. 
Art 7. The Problem propofed is, Why Bodies 
diffolved float in Liquors lighter than themfelves ? 
as for Example: Mercury diflolved in ftrong 
Spirit. of Nitre fwims therein, tho’ each fmall 
Particle of Mercury, be far heavier than fo 
much of the Liquor whofe place it occupies. 
This, fays he, cannot be folved by the prime 
Law of Hydroftaticks, which is, that a Bo-. 
dy which is an equal quantity is heavier than 
a like quantity of Liquor, finks in that Li- ® — 
: : quor ; 


“ 


- Maifcellanea Curiofa. 201 
‘quor ;: thus a Cubick Inch of Iron being hea- 
vier than a Cubick Inch of Agua-Fortis, and 
each Particle (how fmall foever) of Iron be- 
- ing heavier than a like Particle of Agqua-Fortis 5 
Iron being put into iAgua-Fortis fhould fink, 
and yet we find, that Iron being diffolved in 
a convenient quantity of Agua-Fortis floats 
therein, and does not fall to the Bottom. 
The Reafon which my Brother gives for this 
is, That the internal Motion of the Parts of 
the Liquor, does keep up the Particles of the 
diffolved Solid, for they being fo every Mi- 
nute, are movable by the leaft force imagi- 
nable, and the AGion of the Particles of the 
Menftruum, is fuiicient to drive the Atomes 
of the diffolved folid Body from place to 
place; and confequently, notwithftanding 
their Gravity, they do not fink in the Liquor 
lighter than themfelves. Asa Proof of this 
in the 7th Article of Fanvier 1685. he offers 
an Experiment known in Chymiftry, that a 
_ Menftruum over a digefting Fire (as the Chy- 
mift {fpeaks) will diffolve a greater quantity 
of a Body put into it, than when ’tis off the 
Fire, andif it be taken offthe Fire, and fuf- 
fered to cool, a great Portion will precipi- 
tate of that which was perfe&ly diflolved, 
whilft the Afenftruum continued hot. | For, 
fays be, the Particles pf the ALenfruum ac- 
quire a more violent agitation by the Fire, 
and are therefore able to raife and. keep up 
a greater Quantity of the diflolved Body, or 
hereby they are able to refift a greater Gra- 
vity. | 
it has been objected againit this Notion, 
that the common Experiment of precipita- 

tion, 


— 


202 Maifcellanea Curwfa.  - 
tion, by mixing an Alkaly with an Acid feems — 
to contradi& this; for thereby the Fluidity | 
of the Aenftruum is not taken away, and 
confequently, the internal Agitation of its 
Parts is not diminifhed, and yet thereupon, 
the Particles of the diffolved Body precipi- 
tateall to the Bottom. ‘To this he anfwers 
in the forecited Article of Fanuary, that all 
Mixtures of different Liquors introduce in 
each a different Conformation of Pores, and > 
therefore the Infufion of a new Liquor, drives 
the infefible Parts of the diffolved Body from 
their Places, and forces them to ftrike a- 
gainft each other, and cling together, and — 
fo becoming more big aad heavier tha. for- 
merly, the internal Agitation of the Liquor 
is no longer able to move and fuftain them, 
and confequently theyfall to the Bottom. 

This, as fairly and fhortly as I can propofe 
it, is his Sentiment of this Phenomenon. 

But I conceive an other.-Account may be 
given of this Appearance, and that the fore- — 
faid Law of Aydroftaticks is alittle deficient. - 
Tis true indeed, if we confider only the fpe-- 
cifick Gravity of a Liquor, and the fpecifick 
Gravity of a folid Particle floating therein, 
the forementioned Rule is exact; but in 
finking there is requifite a feparation of the 
Parts of the Liquor by the finking Body; and 
there being a natural Inclination in the Parts 
of all Liquors to Union arifing from an A- 
greement or Congruity of their Parts, there 
isa refiftance therein to any thing that fe- 
parates this Conjunction: Now unlefs a Bo- 
dy have weight enough to overcome this 
Congruity or Union of Parts, fuch a Body 

will 


_ Maifcellanea Curiofa. — 303 
will float in a Liquor fpecifically lighter than 
it felf. But that a heavy Body, as Adercury 
or /ron may. have its Parts reduced to that 
Minutenefs, that their Gravity or Tendency 
downwards, is not ftrong enough to feparate 

'the Cohefion or Union of the Parts of a Li- 
quor, will be manifeft, if we confider, that 
the Refiftance made by the Afedium to a fal- 

- ling Body, is according to the Superficies of 
the Body; but asthe Body decreafes in Bulk, 
its Superficies does not proportionably de- 
creafe, thus a Sphere of an Inch Diameter, 

- has not eight times lefs Superficies than a 
Sphere of two Inches Diameter, tho’ it have 
eight times lefs Bulk, and confequently paf- 
fing through a Adedivm, as fuppofe Air or 

~ Water, the Sphere of an Inch Diameter is, 
proportionably to its Bulk, more refifted, than 
a Sphere of two Inches Diameter in propor- 
tion to its Bulk, and hence it will come to 

-pafs, that at laft a Body may be reduced to 
that Minutenefs, that its Gravity prefling 
downwards (which is according to its Bulk) 
may be lefs than the refiftance of the Aé¢edi- 

‘um, which operates on the Surface of the 
Body; feeing as I faid before, the Surfaces 
of Bodies do not decreafe fo faft as their 
Bulks, thefe decreafing in a Triplicate, but 

—thofe in a Duplicate Ratio,of the Bodies Dia- 

- meters. 

This Account does not at all oppofe the 
Experiment of a Menftruum over the Fire, 
being able ta diflolve or fuftain a greater 
Quantity of a heavy Body; for the Reafon, 
of this, as’tis given by my Brother, does not 
Contradi¢t my Notion. The Account nes 

: wife 


ie -: Mifjedlamee Curiofel 
wife, that He gives of Chymical Precipita- | 
tion agrees very well with what} propofe : 
So that of thefe I fhall fay no more. : 

But becaufe in the beginning of my Dif 
courfe, I fay that the forementioned: Law of 
_ Hydroftaticks isa little defective, 1 defire toex-. 
plain my felf a little further in that Point. In 
Weights falling through the Air, were Gra- 
vity only confider’d, the Proportions of their 
Defcents would be exadtly as Galileo has de- 
monftrated ; but it is allow’d by-all, that the 
Refiftance of the Air, not being. confider’d in 
thofe Demonftrations, they are not Mathe- 
matically true in Praétife, but that really 
there is fomething of that proportion hind- 
red by the Airs Refiftance. Now, what is 
this lefs than to fay, that the Refiftance of 
the Air takes off fome of the Operatien of 
Gravity, or is able to withftand or oppofe 
part of its AGion? And if fo, what fhall we 
fay were an Iron Sphere let through a Me- 
dium of Water? Surely the Proportions of 
its defcents would be much more difturbed 
herein, as Water is much more Solid and dif- 
ficult to be feparated or pafled through than 
Air; and confequently we muft needs grant, 
that more of the Operation of Gravity, is 
_ taken off or refifted by this Oppofition of the 
Water, than that of the Air. And. if fo,. 
furely there may be a certain degree of Gra- 
vity,; that may be quite taken off by the 
_refiftance of the Water: Were a Piltol Bul- 
Jet let fall through the Air, it would defcend 
imperceptibly nigh the Propor tions that Ga- 
fileo has afligned, but were a fingle grain 
of Sand fo let fall, it would-be much hiadred 

in 


” 


“3 
i - 
i 44 


Maifcellanea Curiofa. 205 


in its Courfe, and the half of this Grain would 
be more obftructed ; what fhall we then fay ~ 
of the ten thoufandth part, or of a part the 


ten thoufand millioneth of this, and agai of 
the Infinits Subdivifions of that, till at laft 
we come to a part that would be wholly re- 


Sifted, or kept up; fuch as I conceive the 


‘minute Particles of a Body diffolved in a 


Menftruum ? tae es 
- On this account ’tis, 1 fay, that the fore- 
mentioned Principle of Aydrofraticks is a little 


defective; for it confiders not the natural’ 


Congruity of the Parts of a Liquor, whereby 
they defire, as *twere, to unite and keep to=- 


gether, juft as we fee two drops of Water on ~ 
‘adry Board being brought together do jump 


and coalefce, and therefore Liquors have an 
innate power of refifting a certain degree of 
force that would feparate them; fuch as I 


fuppofe the degree of Gravity, in the moft 


minute Particles of a Body diffolved ina 
Menftruum. 7 ; 
_ The fore-mentioned Rule holds true to the 
moft nice Senfe in great Bodies, but in thofe 
that are by many Millions of Divifions {mal- 
ler, it feems to fail. he | 
“This, in fhort, is my Conjefture in this 
matter, which I propofe, as my Brother did 
his, with all fubmiffion imaginable, and there 
by to give occafion to others to enquire into 
‘the Caufes of this appearance, rather than to 
publifh my own Sentiments as the undoubted 
Solution thereof. eee 
But this 1 muft acknowledge, that the in- 
ternal motion of the parts of a Liquor feems 
fo very agreeable to truth, and explicates fo 
| ° 4 many 


306 = Mifcellanea Curiofa. 
many Phenomena eafily and plainly, that I 
would not be thought to deny it. Neither 
would I be thought wholly to reject my Bro- 
thers Solution of this Problem 3 for certainly 
that Motion (whatfoever it is) in a A/en- 
 flruum, which is able to diffolve fuch a folid 

‘Body as Iron, that is, which is able to di- 
fturb the clofe and ftrong Cohefion of the 
Parts of Iron, may very well be fuppofed fuf- 
ficient to difturb or keep up thefe parts from 
refting in the bottom of the Veffel, wherein 
the folution was made: And certainly no 
better account can poflibly be given of fuch 
Solutions, than by fuppofing fuch an internal 
motion in the parts of the Adenftruwm infinu- 
ating themfelves into the folid Body, and 
loofening its parts. And tho’ it may be ob-. 
jected, that in the parts of Water there may 
be fuppofed as violent an internal motion, as 
in the parts of Aqua-Fortis, and yet we fee 
Water will not diffolve Iron as Aqua-Forte 
does, and common Bees-Wax is difturbed by 
neither of them, I leave the nice enquiry 
after this Point to others, wiz. What kind of 
Motion and peculiar Conformation of parts 
is requifite both in the Adenftruum and in the 
diffolved Body, that a Solution may refult 
from their Commixture. Rieti dt , 


Some Reflections on the foresoime 
Paperby, dio kee ata 

What my Brother has laid- down in this 
Difcourfe,; [think does moft undeniably evince 
that the received Law of Alydroffaticks is 
‘Aomewhat detective. For Liquors, tho’ they 
fl ia * r are 


| Mifcellanea Curiofa. 307 
are Fluid yet they are Bodies, and therefore 
confift of parts united 3 which Union, tho’ it 
be eafily deftroy’d, yet of neceflity it requires 
fome degree'of Force for the efleGting it; nor 
is it more manifeft, if rightly confidered, 
that a Flint requires Force for the feparation 
ef its parts, than that Fluids do for theirs. 
But however, I imagine, this Property ought 
not to be relied upon as the fole Caufe of this 
appearance, to which my Brother has apply’d. | 
it; nay perhaps does not fo muchas concur 
the leaft in the producing this effect; my 
Reafon in fhort is this: Whatever is of fuff- 
cient Power to raife the minute Particles of 
a heavy Body in a light Fluid, is certainly a 
fufficient caufe to keep them in that ftate : 
Now my Suppofition may give fome account 
of this, what my Brother fays, never can 3 
for he muft neceflarily fuppofe them firft 
raifed ; and then he gives the reafon of their 
not finking: Whereas ’tis not to be quefti- 
oned but that that Force which raifed them, 
is the fame which keeps them from falling to 
the bottom. 

But thefe Conjefures (for I efteem them 
no more)! leave to the Confideration of thofe 
that defire to enquire further in this Mat~ 
eer. 


¢ 


1 ag? Mnifcellanea sir | 


of Of the aveig ht of a ole foot of er 

vers grams, &c. try’ "ama Vef- 
fel of well-feafon’'d Oak, whofe 
concave eons an cnt cape foot. 
By the direction of the Philofo- 
phical Society at Oxford. | 


HE following Bodies were poured 

gently into the Veffel, and thofe in the 
12 firft Experiments were weighed in {cales 
turning with 2 ounces, but the laft 7 were 
weigh’d in feales turning with one ounce. 
The pounds and ounces here mentioned ‘are 
Avoirdupois. 


, 7 aa, a ae 
1. A foot of Wheat (worth 6s.a - 
Bufhel ) weigh’d of Avoirdupois_ 
weight. 47. 8 
ae ers of the beft fort (worth 
4.4. a Bufhel) 43. de 
3. “Che huh fort of Wheat meafured . 


a fecond time. Oo. ae 
Both forts were red Lammas Wheat of 4 
the laft year. 
4. White Oats of the laft year. 29. © 
The beft fort of Oats were 2d. ina 
Bubhel better than thefe. 
5- Blue Peafe (of the laft year) and 
much worm-eaten. | 49. 1% 
6. White Pea/e of the laft year but one. 50. %. 
q. Barley 


. Mifcellanea Curtofa. 309 
| ib. 3. 


», Barley of the laft year (the beft 
fort fells for 1s. 6d. ina Quarter 


more than this. : Als 2. 
8. Malt of the laft years Barley, made 

2 Months before. 130. % 4. 
9. Field-Beans of the laft year but one. 50. 8. 
10. Wheaten AZeal (unfifted). St. Ge 
11. Rye Aeal (unfifted.) wgB. fe 
12. Pump Water. 62. 3%. 
13- Bay Salt. 34. 1 
14. White Sea-Salt. 43: 2. 
rg. iSand.. 85. ge 
16. Newcaftle Coal. G7. 2. 


17. Pit-Coal from Wednesbury, 63: 
but this is very uncertain in the 
filling the Interftices betwixt the 


“greater pieces. 63. 0. 
18. Gravel. | 109. §. 
19. Wood-Afhes. 3 58. 5. 


A further Lift of the Specifick Gravities of 
Bodies, being in proportion as the following — 
numbers. 


ee. 7000 
Fir dry 546 
Elm dry 600 
Gedar dry Ol 
Walnut-tree dry - 631 


Crab-tree meanly dry | 
Ah meanly dry, and of the out-fide lax 
part of the Tree 734. 
Afhmore dry, but about the Heart 845 
Maple-tree e855 
: X 3 Yew 


7645 


2 10 Mifcellanea Curiofa. 


“Yew of a Knot or Root 16 years old 760 


Beech meanly dry W854 
Oak very dry, almoft Worm eaten 133 
Oak of the out-fide fappy Betts fell’d a 
year fince 870 
Oak dry, but of a very found ‘clofe tex- 
LUEE 2 — 929 
The fame tried another time 932 
Logwood SEO OLS 
Claret : nye id eu QOS 
Moil Cyder not clear | 1017 
Sea-water fetled clear He Ose 
College plain Ale the fame : 1028 
Urine | 1030 
Milk | t aedt. DORE 
Box the fame ~ . 1031 
Redwood the fame es LOSE: 
sack Jh2tO33 
Beer Vinegar vey 1034 
Pitch i J115@ 
Pit-Coal of Stafford- fhite : ¥240 
Speckled wood of Virginia Stee G 
Lignum Vite — pL a27 
Stone-bottle C7 Lae 
‘Ivory : . 1826 
Alabafter : 1872 
Brick | ° 1979 
Heddington-ftone, . foft lax kind. 2029 
Burford-ftone, an old dry piece *") ¥)g0a8) 
Paving-ftone a hard fort from about | 
Blaidon t 2460 
Flint 7 2542 
Glafs of a quart Bottle, > 2666 
Black Italian Marble 2704 
Ww hite Italian Marble tried twice . 2707 


White 


—— MifeeNanea Curiofu. = 311 


White Italian Marble of another fort 


of a vifibly clofer texture 2718 
ppiock-tin re / 7321 
Copper ae : $843 
Lead ye 11345 
Quick-filver 14019 
Quick-filver 2 ee es 


The laft Experiment was tried with another 
quantity of Quick-filver, which had been 
ufed in Water in the preceding Experiment: 
However I rather truft the laft, for that I 
found a fimall miftake (tho’ here in the cal- 
culation allawed for) in the weight of the 
Glafs containing the Quick-filver in the trial 
before. a 
The Solids here mentioned were exami- 
ned hydroffatically by weighing them in Air 
and Water; but the Fluids, by weighing an 
equal portion of each ina Glafs holding about 
a quart. The numbers fhew the proportion 
of gravity of equal portions of thefe Bodies ; 
but if of thefe Bodies we take portions 
equally heavy, their magnitudes will be reci- 
procally proportional to their correfpondent 
numbers, e,g.a cubic foot of water isto a cubic 
foot of Alabafter in gravity as 1000 to 1872; 
but a pound weight of water, is toa ponnd 
weight Albafter in magnitude as 1872 to 1000. 
So that knowing by the former Table the 
weight of acubic foot of Water, and by this, 
the proportion in gravity betwixt Water 
and Alabafter, we may by the Rule of Three 
find the weight of a cubic foot of Alabafter, 
and fo of any other of thefe Bodies ; or we 
‘may know their magnitude by knowing their 


X 4 : gla~ 


giz Mifcellanea Curiofa. 

gravity. Sothat an irregular piece or quan- 
tity of thefe Bodies being offered, *tis but 
weighing them, and we may know their juft | 
magnitude without further trouble. 


Obfervations of the Comparative, Intenfive 
or Specific Gravities of various Bodces. 
Made by Mr. J. C. ; | 


Ump-water, — Ag 1000 
Cork, ce fe 2.37 
Saflafras Wood, it ‘ 482 
Juniper Wood (dry) ~ ‘> §56 
Plum-tree, (dry) 663 
Maftic, : 849 
Santalum Citrinum, : 809 
Santalum album, 1041 
Santalumrubrum, 1128 
Ebony, : L177 
Lignaum Rhodium, - yo eae 
Lignum Afphaltum, : 1179 
Aloes, | 1177 
Succinum pellucidum, oes (Ge 
Succinum pingue, : 1087 
Jet, 1238 


The top part of a Rhinocero’s horn, 1242 
pp iT, +2 


‘The top part of an Ox horn, os us a OAC 
The (Blade) bone of an Ox, \ +S 
An human Calculus, 1240 
Another Calculus humanus, me 
Another Calculus, ° 1664, 
Brimftone, fuch as commonly fold, 1815 
Borax, — Wigs te 172Q: 
A fpotted faGtitious Marble, 1822 
& Gally-Pot,) 1 tain : 1929 
Lue sa Oylter- 


Mifcellanea Curiofa. 


Opter-ihell,, 
Murex-fhell, 

Lapis manati, 
Selenitis, 


- Wood petrefied in Lough-Neagh, 


Onyx-ftone, 
-Turcois-ftone, 

Englifh Agat 
Grammatias lapis, 

A Cornelian, © 
_Corallachates, 

Tale. 

Coral, 

Hyacinth (fpurious) 
-Jafper ({purious) 

A pellucid Pibble, 

Rock Crytftal, 

Cryftallum Difdiaclafticum 
A red Patfte, : 
Lapis Nephriticus, 

Lapis Amiantus from Wales, 
Lapis Lazuli 7 

An Hone, 

Sardachates, 

A Granat, 

A Golden Marcaiite, 


9 


_ Ablue Slate with fhining Particles, 
A mineral Stone, yielding 1 part in 


160 Metal, 


The Metal thence extra¢ted, 
The (reputed) Silver Ore of Wales, 
The Metal thence extracted, 


Bifmuth, | 
Spelter, . 

Spelter Soder, 
Tron of a Key, 


es} 


2092 
2590 


2290 


2322 
2345 
2510 
2508 
aSlz 
2515 


- 2568 


2605 


2657 
2689 


‘2635 


2666 
264% 
2659 
2704. 


“42842 


2894 
2913 
3054. 
3288 
3598 
3978 
4589 
3500 


2650 
8500 
7404 
LIO87 
9859 
7O6§ 
3362 
7943 


Steel, 


Steel, 

Caft Brafs, 

Wrought Brafs, 

Hammer’d Brafs, 

A falfe Guinea, 

A true Guinea, 

Sterling Silver, 

A brafs Half-Crown, 
Ble4trum, a Britifh Coin, 

A Gold Coin of Barbary, 

A Gold Medal from Morocco, 
A Mentz Gold Ducat, 

A Gold Coin of Alexanders, 

A Gold Medal of Queen Mary, 
A Gold Medal of Queen Elizabeth, 


214. Mifcellanea Curiofa. 


7852 


“8100 


8280 | 
3349 
9075 
18888 
10535 
9468 — 
12071 


17548 


18420 
18261 
bhoreys | ue 
19100 | 
19125 


A Medal efteem’d to be near fine Gold, 19636 | 


— Mifcelanea Curiofa. 315 


o 2 HERO Laa 


yee! * 

A Letter of Dr. Wallis to Dr. 

Sloane, concerning the Generation 
of Hail, and of Thunder and 
Laghtning,and the Effects thereof. 


Z 


Oxon. Fuly 26.1607. 

STR july 97 
] Thank you for the TranfaGtions of Fuze 

_ which you fent me; wherein I am well 
pleafed with Mr. Haley’s Remarks on the 
Torricellian Experiment at the top of Szom- 
don-hill in Wales, at the height of 1240 yards 
perpendicular. Where the height of that 
Quickfilver in the Barofcope was 3 Inches 
and f. lefs than below at the Sea-fide; \ which 
is an Obfervation of good ufe ; and would 
have been more fo, had he had the leifure to 
make like Obfervations at feveral other per- 
-pendicular. heights in the Afcent. For 
from fuch comparative Obfervations we are 
to make an Eftimate, at what proportion the 
height of the Quickfilver doth decreafe in re- | 
ference to the height of the place. I mean 
_ whether in the fame Proportion, or the Du- 
plicate, Sub-duplicate, or how otherwife 
Complicate thereof. From whence we may 
make a Judgment of the height of the Atmof~ — 
phere, if at leaft it have a determinate 
height. I did once attempt (a great while 
fince) a.Computation of it; but wanted a 
fafficient number of Dara to proceed upon 
Hh ey : ut 


~ 


216  Mifcellanea Curiofa. 
But that which is moft furprizing in thofe 
TranfaGtions is, the prodigious Aas there 
mentioned , which happen’d at many Places, 
on different Days, and all within the compafs 
of lefs than fix Weeks. I have been told of 
the like in other Places about the fame time, 
in Lincolnfbire, Hampfhire, and elfewhere ; 
whether or no on the fame Days which you 
mention, I cannot tell; nor can I give a par- 
eicular Account of them. But it would be 
kind in thofe who can, to give you like Ac- 
counts thereof with thofe you have Publifhed, 
for a like publick Information. 
I find it is thought very ftrange, what 
fhould caufe fo fudden a Congelation of Hail-- 
ftones to fo great a bignefs before they fell. 
And it is indeed very ftrange. But it is not 
neceflary that the whole bignefs be attained 
before they begin to fall, but the freezing 
may continue during the Fall, to increafe the 
Bulk. For I remember that (many Years 
fince) I obferved here at Oxford a ftrange — 
fhower of Hail, wherein (befides the formed - 
Stones that fell on the Ground, there did 
hang on the Treesa great deal in the Form 
of Icicles (a Foot or more in length) fo 
many and heavy, as to break off fome Boughs 
with their weight ; and I was then told, that 
in fome places great Branches of Trees were 
fo broken off; which muft needs be from the 
continuing to freeze during the fall. 


And truly the Generation of Hail in ge- 
neral, isa thing which deferves to be farther 
inquired into, than (I think) hath been yet 
done. I find Mr. Haley (in his Narration) 

Ae afcri- 


Mifcellanea Curiofa. 317 
afcribing it to Vapour difpofing the Aqueous 
Parts fo to congeal.. And not unlikely. 
If I may interpofe my Opinion, you may 
take it thus: | | 
Thunder and Lightning are fo very like the 


Effects of fired Gun-powder , that we may 


reafonably judge them to proceed from like ~ 
Caufes. The violent Explofion of Gun- 
powder, attended with the Noife and Flath, 
is fo like that of Thunder and Lightning, as 
if they differed only as Natural and Artifi- 
cial, as if Thunder and Lightning were a 
_ kind of natural Gun-powder, and thisa kind 
of artificial Thunder and Lightning. : 
_ Now the principal Ingredients in Gun- 
powder are, Nitre and Sulphur (the Admi- 
ftion of Charcole being chiefly to keep the 
Parts feparate for the better kindling of it.) 
So that if we fuppofe in the Air, a conve- 
nient mixture of Nitrous and Sulphorous Va- 
pours, and thofe by Accident to take Fire ; 
fuch. Explofion may well follow, with fuch 
Noife and Light, asin the firing of Gun-pow- 
der. And being once kindled, it will run on 
from Place to Place as the Vapour leads it, 
‘as in a Train of Gun-powder, with like _ 
Effects. 

This Explofion, if high inthe Air, and far 
from us, willdo no Mifchief, or not confider- 
‘able; like a parcel of Gun-powder fired in ~ 
the open Air, where is nothing near to be 
hurt by it: Butif near, to us (or among us) 
it may kil] Men or Cattle, tear Trees, fire 
Gunpowder, break Honfes, or the like; as 
Gun-powder would do in like Circum- 
ftances. 3 

Now 


218 Maifcellanea Curiofa. 

Now this nearnefs or farnefs may be eftimated 
by the Diftance of Time between feeing the 
Flafh of Lightning, and hearing the Noife of 
the Thunder. For though in their Genera- 
tion, they be fimultaneous; yet (Light mov- 
ing fafter than Sound) they come to us fuc- 
ceflively. I have obferv’d that; commonly; 
the Noife is about Seven or Hight Seconds 
after the Flath (that is, about half a quarter 
ofa Minute); but fometimes mueh fooner, in 
a Second or Two, or lefs than fo; and almoft 
immediately upon the Flafh. And at fuch 
time, the Explofion muft needs be very near 
us, or even amongft us. And, in fuch Cafes, 
1 have. (more than once) prefaged the Ex- 
pectation of Mifchief, and it hath proved ac- 
cordingly, in the Deftru@ion of Men or Cat- 
tel, andthe like. (As once at Oxford; when, 
within half an Hour after fuch Prefage, I 
heard of one killed at, AZedly, hard by, and 
others endangered ; and another time at Tow- 
cefler, when within a few Hours after, we 
heard of Five Perfons kil?d at Everton, about 
Four or Five Miles from us, and others 
wounded ; befide other Hurt done.) 

Now, thatthere is in Lightning a Sulphor- 
ous Vapour, is manifeft from the Sulphorous 
Smell which attends it, efpecially when Hurt 
is done; and even where no Hurt is done, 
fromthe Lightning it felf,more orlefs difcern- | 
able. Anda fultry Heat inthe Air, is com- 
monly a Fore-runner of Lightning foon after. 

And that there is alfoa Nitrous Vapour 
with it, we may reafonably judge, becaufe we 
do not know of any Body fo liable toa fud- 
dain and violent Explofion. | 

Now 


Mifcellanea Curiofa. 219 

‘Now thefe Materials being admitted, it 
remains to be confidered, how they may be 
kindled in order to fuch Explofion. As to 
which,I have been told from Chymitts (though 
I have not feen it tried) That a Mixture of 
Sulphur, Filings of Steel, with the Admiffion 
of a little Water, will not only caufe a great 
Effervefcence, but will of it felf break forth 
into an actual Fire. 

So that there wants only fome Chalybeat 
_ or Vitriolick Vapour (or fomewhat equivalent) 
to produce the whole Effe& (there being no 
want of Aqueous Matter in the Clouds.) | 

And there is no doubt, but that amongft 
the various Effluvia from the Earth, there 
may be copious Supplies of Matter for fach 
Mixtions. 

And ’tis known, that Hay, if laid up too 
Green, will not only heat, but take Fire of 
it felf. | 

And while we are difcourfing of this, it may 
fuggeft fomewhat as to the Generation of Hail 
_ which is very oft an attendant of Thunder 
‘and- Lightning. .’Tis well known, in our ar- 
tificial Congelations, that a Mixture of Snow 
and Nitre (or even common Salt) will caufe 
a prefent and very fuddain Congelation of 
Water. And the fame in Clouds may caufe 
that of Hail-ftones. Andthe rather, beeaufe 
(not only in thofe prodigioufly great, but in 
common Hail-ftones) there feems fomewhat 
like Snow rather than Ice, in the midft of 
them. | 

And, as to thofe in Particular (of which we 
are now fpeaking) fo véry large (as to weigh 
Halt a Pound, or Three Quarters of a Pound) 

fup- 


Ms a a Reid nk Se dN DN a i i ta 


220 MifceHanen Curiofa. — 
_ fuppofing them to fall from fo great a Height, — 
as tis manifeft they did by tne Violence of 
their Fall: ’Tis very poflible, that though ~ 
their firft Concretion, upon their fuddain 
Congelation, might be but moderately great, 
asin other Hail; yet, in their long Defcent, 
if the AZedium through which they fall were 
alike inclined to Congelation, they might — 
receive a great Acceffion to their Bulk, and 
divers of them incorporate into one Like as 
in thofe Icicles before mentioned. 

Thefe have been my Thoughts, occafioned 
by the Confideration of the furprizing Great- 
nefs of thefe Hail-ftones, with the great 
Thunder and Lightning which did atten 
thefe Storms. - | | 


Yours, &c. 


THE 


a Ft 
a 


, Fi ; ra i : 
7 , ee \ Fi ae 
i ya * f 
i = ‘ J ‘ 
‘ £ y 7 
= af . / 
bs a | ; fe e 
; , fs ’ : a ow , é 
€ \ a 
é : . ; t fe ° if 
, ~ S 7 ' Pee 
, A ; A ' 
ey y ep 1 ? 
F t 
; : | i 
f i 5 \ I ae i 
. ~~ i 
% oy ‘ : : I 1 
% 4 
; ; F ’ 1 i ¢ 
f ' ; \ 
J 4 ‘ i 
t : b ‘ 
f ‘3 : 1 H 
5 A { 4 Bt 
wo ’ D \ s 
‘ y \ 
7 < : ; f re: 
= a \ . 
, 
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- It . 
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2 . 
) ( 
‘ ‘ = 
ch a 
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j , mi < 
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\ { 


SYNOPSIS 
Aftronomy of Comets. 


HE ancient Egyptians and Chaldeans 

Cif we may credit Diodorus Siculus) 

by a long Courfe of Obfervations, 

were able to predict the Apparitions 

6f Comets. But fince they are alfo faid, by 
the Help of the fame Arts, to have prognolti- © 

cated Earthquakes and Tempetts, ’tis paft ail 
Doubt, that their Knowledge in thefe Matters, 
was the Refult rather of meer -4ffrological Cal- 
culation, than of any Aftronomical Theories of the 
-Ceeleftial Motions. And the Greeks, who were 
the Conquerors of both thofe People, fcarce — 
found any other fort of Learning amongit 
them, than this. So that ’tis to the Greeks 
fhemfelves as the Inventors (and efpecially to 
the Great Hipparchus) that we owe this Affro- 
nomy, Which is now improv’d to fuch a Heigth. 
But yet, among{t thefe, the Opinion of Ari- 
ftotle (who wou’d have Comets to be nothing 
elfe, but Subluaary Vapours, or Airy Meteors) 
: Bes pre- 


6 Mifcellanea Curiofa.. 
-prevail’d fo far, that this moft difficult Part 
of the Aftronomical Science lay altogether neg- 
lected ; for no Body thought it worth while 
to take Notice of, or write about, the Wan- 
dring uncertain Motions of what they efteemed 
Vapours floating in the e€ther , whence it came 
to pafs, that nothing certain, concerning the 
Motion of Comets, can be found tranfmitted 
fromthem tous. pe het af 
But Seweca the Philofopker, having confider’d 
the Phazoimena of Two remarkable Comets of 
his Time, made no Scruple to place them a- 
mongit the Celefial Bodies; believing. them 
to be Stars of equal Duration with the World, 
tho’ he owns their Motions to be governd by 
Laws not as then known or found out. And at 
laft (which was no untrue or vain Prediction) 
he foretells, that there fhould be Ages fometime 
hereafter, to whom Time and Diligence fhow’d 
unfold all thefe Myfteries, and who fhou’d 
wonder that the Ancients cou’d be ignorant of 
them, aiter fome lucky Interpreter of Nature 
had fhewn, zz what Parts of the Heavens the Co- 
mets wanderrd, what, and how great they were. 
Yet almoft all the Aftronomers differ’ from 
this Opinion of Sezeca;. neither did Sezeca him- 
felf think fit to fet down thofe Phenomena ot 
the Motion, by which he was enabled to maintain ~ 
his Opinion: Nor the Times of thofe Appear- 
ances, which might be of ufe to Pofterity, in 
order to the Determining thefe Things. And 
indeed, upon the Turning over very many 
hiftorics of Comets, I find nothing at all that 
can be of Service in this Affair, before, 4. D. 
1337. at which time Nicephorus Gregoras, a Con- 
feantinopolitar Hifterian and Aftronomer, did 
oe pretty 


My{cellanea Curiofa. 2 
pretty accurately defcribe the Path of a Comet 
amongit the Fix’d Stars, but was too laxe as 
to the Account of the Time; fo that this moft 

. doubtful and uncertain Comet, only deferves to 

be inferted in our Catalogue, for the fake of its: 
appearing near 400 Years.ago. ~ 

Then the next of our Comets was inthe Year 
1472,Which being the {wifteft of al],and neareft 
to the Earth, was obferv’d by Regiomantanus. 
This Comet (fo frightful upon the Account 
-bothof the Magnitude of its Body,and the Tail) 
mov d Forty Degrees of a great Circle in the 
Heavens, in the Space of one Day; and was 
the firft, of which any proper Obfervations 
are come down to us. But all thofe that 
confider'd Comets, until the Time of Ticko 
Brabe (that great Relftorer of Aftronomy) 
believ’d them to be below the Moon, and fo 

took but little Notice of them, reckoning 
them no other than Vapours. 

But in the Year 1577, (Ticho feriorfy 
purfuing the Study of the Stars, and having 
gotten Jarge Inftruments for the Performing 
Cocleftial Menfurations, with far greater Care 
and Certainty, than the Ancients cou’d ever 
hope for) there appear’d a very remarkable 
Comet ; to the Obfervation of which, Trecho 
-vigoroufly applied bimfelf; and found by ma- 
ny juft and faithful Trials, that it had not a 
Diurnal Parallax that wasat ail perceptible: 
And confequently was not only no Aircal Va- 
pour, bat alfo much higher than the Moon ; 
nay, might be plac’d amongit the Planets. for 
‘any thing that appeard to the Contrary , 


the cavilling Oppofition made by fome of the 
Bie oe A 2 School- 


4  Mafcellanea Curiofa. 
School-men in the medn time, being to no Pur- 
pofe. eo ! hae 
Next to Ticho, came the Sagacious Kepler. 
He having the Advantage of Ticho’s Labours 
and Obfervations, found out the true Phyfical — 
Syftem of the World, and vaftly improv’d the 
 Aftronomical Science.. aa ae 
For he demonftrated that all the Planets per- 
form their Revolutions in Eliptick Orbits, whofe 
Plains pafs thro’ the Center of the Sun, obferving 


-‘thisLaw, That the Area’s (of rhe Elliptick Settors, 


taken atthe Center of tke Sun, which he proved 
to be in the common Focus of thefe Ellipfes) are 
always proportional to the Times, in which the cor= 
refpondent Elliptical Arches are deferib'd. He 
difcover’d alfo, That the Diftances of the Pla- 
nets from the Sun are in the Sefquialtera Ratio 
of the “Periodical Times, or (which is all 
one) That the Cubes of the Diftances are asthe — 
‘Squares of the Times. This great Aftronomer — 
had the Opportunity of obferving Two Co- 
mets, one of which was very remarkable one. - 
And from the Obfervations of thefe (which af- 
forded fufficient Indications ofan Annual Paral- 
lax) he concluded, That the Comets mov'd freely 


‘thro? the Planetary Orbs, with a Motion vot much 


different from a Rettilinear one, but of what Kind 
he coud not then precifely determine. Next, He- 
welius (a Noble Emulator of Ticho Brabe) fol- 
lowing in Kepler’s Steps, embraced the fame 
Hypothefis of the Reéctilinear Motion of Co- 
mets, himfelf accurately obferving many of 
them. Yet, he complaind, that his Calculations 

did not perfectly agree to the Matter of Fa& 

in the Heavens: And was aware, that the Path: 
of a Courct was bent into a Curve Line towards the 


Sarr. 


| Mifcelanea Curtofa. 5 
Sun. Atlength, came that prodigious Comet 
of the Year 1680. which defcending (as it were) 
_ from an infinite Diftance Perpendicularly towards 
the Sun, arofe from him again with as great 
a Velocity. ts 

This Comet, (which wasfeen for Four Months 
continually) by the very remarkable and pe- 
culiar Curvity of its Orbit (above all o- 
thers) gave the fitteft Occafion for inveftiga- 
ting the Theory of the Afoticn. And the Royal 
 Obfervatories at Paris and Greenwich having been 
for fome time founded, and committed to the 
Care of molt excellent Aftronomers, the. appa- 
vent Motion of this Comet was molt accurately 
(perhaps as far as Humane Skill cou’d go) ob- 
ferv’d by Mrs. Caffiné and Flam/teed. z 

Not long after, that Great Geometrician, the — 
Tlluftrious Newton, writing his Mathematical 
Principles of Natural Philofophy, demonitrated 
-not only that what Kepler had found, did ne- 
ceflarily obtain in the Planetary Syfiem, but al- 
fo, that all the Phexomena of Comets woud 
naturally follow from the fame Principles; 
_ which he abundantly illuftrated by the Exam- 
ple of the aforefaid Comet of the Year 1680. 
fhewing, at the fame time, a Method of Deli- 
neating the Orbits of Comets Geometrically ; 
wherein he (not without the higheft Admirati- 

on of all Men) folv’d a Problem, whofe Intrica- 
cy render’d it worthy of himfelf. This Comet 
he prov'd to move round the Sun ina Parabo- 
lical Orb, and to defcribe Area’s (taken at 
the Center of the Sun) proportional to the 
Times. | | 


A3 Wheres 


6. Mafeellanen Curtofad = 


Wherefore Cfollowing the Steps of fo Great « 

Man) have attempted to bring the fame Me- 

thod to Arithmetical Calculation, and that with — 
defired Succefs. For, having collected all the - 
Obfervations of Comets I could, I fram’d 
this Table, the Refult of a prodigious deal of 
Calculation, which, tho’ but fmallin Bulk, will — 
be no unacceptable Prefent to Aftronomers. For 
‘thefe Numbers are capable of Reprefenting all 
that has been yet obferv’d about the Motion of 
Comets, by the Help only of the following 
General Table, in the making of which I {pard 
no Labour, that it might come forth perfect, 
as a Thing confecrated to Pofterity, and to 
jaft as long as Ajtronomy it fell. PSL 


SS 
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~ &. a 21-14. ¢ Tea 738 169 B 50 7768499). 3119.53 morro e . 8 at 
aS S. {6 LLL9,02 »G CMe Be: 84.750 2:579498)08, 16, 35 83:36:7 ® ebros be YU wo + 
ee me VP 27. 30.3 476.05. gp 41-2 44851 gal Na 2.5 ce clone Retro ass 
S < 71f || = * 1 , ——. oe = & 
x8 1680 M2549 1h on I11-54-30 socal 2.15.40 a 720476 ra ere Cc = = Sy 
ee poe aia ae [3 16.5 10649 cleo 59-5 1.20 iret. | A oO 
3 SY [1683 4 21.36. oleeen be 9-30| 6 ay. 19:22 ee s 1.20 Direct. &) 2 
ee SOS [1683 +1660 |r 56. wate ‘ Sess abject 4.11.52 Fie pe lD ee: we a= 
S 4s,.[168 1 23.23. EEaee st 2805 D834 ‘ee aay, reat. | eee cS 
we Fr Airs Be C 2) Fovd 9.30 9 19 7O\F eb So 7-25)R te =e 
beke eaee ide ae HPA Seti a 152 SET Retrog, 2a84 < 
saiiis. efstatac|eabga. pepe ey tee mean .zoiRetros | 3'E a 
imtsnan 4C m2 9.30 ees Dee, 8 ‘372 29. ol _———— se is = RY q> > 
Yan ML 28.524 —§60 O me 105977 Sept 00, 6 99.12, 5 weet. oO : cs 
$1929-9). 2OOK 9-74.93 ere 4:07 - 9.22 Retrog 2 fas 
70015 }9.982 43) Ful 39 | 108.: 1.301Direét. oe aah 
) 49-9823 39 Mar 3. 250| 8 23 4¢|Retrog 22S ae 
9-10.16 | 7-6 $-ZO}K SEBEL Sees loue 
|..29.22 oo} etrog. be 33 2: | 
oo!D ; Oo 2 0 ° 
Se AUPE es Q: : 
= eet? : ye 
— ee oF Zz Pe < ss ae 
‘ ww ep SS a 


3 = _Maifcellanea Curiofa. é 


A General Table for Calculating the 3 
Motions of Comets in a Parabolic at 
Orbit. 


Med. Ang. a, Logar. Logar. 
mot. |veribelio.| pro dift. pro dift. 
—— |— a Sole. 4 Sole. 

Oo gr, Let es # at bate 


meee | eee ee ore 


| 31 142.55.06]9.062400 
3. 3.15]0,:000309-|| 32 144. 3:2010.065838 
4.34 4310 000694 
6. 6. O|0.001231 


1£2, 7.54}0.004876 
9 |i3.37.17|0.006151 
10 dis, 6: 7|0:007564 


ed 


14 |'16.34.20}0.009115 ‘ 

12 |18. 1.54]0.010798 

13 |19.28.4.7|0.012609 §§ +24 2110.10§ 752. 
14 |20.54.54]0.014550 56.20.12|0.109490 
15 |22.20.14 9.016607 $7:15§+ 6lo.113240} 
16 |23.44.44|0.018783 

17°125. 8.22]0.021072 || 

13 126.31. $19.023470 |! 

19 |27.52.5«|0.025969 69.45.25]0.128278 | 
20. |29.13.4710.028570|| $0 [61.35.45 10.132035 
21. 130.33-4C]o.031263 (\62.25.14]0.135792 


22 31.5 2.32}9.034045 
43°133.10.231o 036916 
24 134.27. 12|9.039864 
_25°135-42.55]9.042892 
26 136.57 411.045989 
27 128.1 1.2019.049154 
28 139.23.54|>.05 2382 
29 |40.35-2 2.055668 | 
20 141 445.4719 o8Qo09 


63.13+52|0.139544 
64. 1-40}o-143291 
64.48.3810.147029 | 
65-34-50|0.1 $0762 
56 66.20 13]0,15.4482 
| 57 \57 04¢50]0.1 58192 | 


$5 


ee 


58 67.48-4210.16 1890] 
59 168-31-50|0.165578 
60 69.14.16}0-169254, 


Mifcellanea Curiofa. 


aun 


0.172914 
70.36.56]0.176557 
71617.1615,180188 


67 173+51-5910.194540 
74.29 5]o.198085 
69 175:05-38]0.201614 


73 17725-51021 5 529 
74 177+59-41)0.218963 
75_|78+32-54 O 222378 


31.41-31]lo.242416 
82.11:T9!0,24.5634 
82.40. 40,0.248933 
83, 9.34.0.252159 
85 {83.38 40-255366 
84. 6. 80.2585 52 
84:33:49 0.261720 
83 485. 1. § 0.264865 
: 85.27.58 0.267989 
85.94.27 0.271092 


Med. 


88.01.27 


Ang. | Logar. 
peribelio, | pro dift 
rome a Sole, 
rg ae 
86.20.34.0.274176 


86.46.200.277239 
87.11.43'0,280284 
87.36.45|0,283306 

0.286308 


————— 


83.25. 4915,289293 
8.49.48'0.292252. 
89.13.320.295201 
89.36.54'0.298122 
79.00-000.301030 
90 4514/0. 306782 
91.29.18)0.312469 


93:34-52/0 329042 
94-14-4010. 334424 
94-5 3+30|0-3 39736 


95-31.2210.344979 
96. 8 22) 350153 


| 99-44.30'0.355262 


97.19.48 0.360306 
97-54°1710.365284 
98. 28 0010. 370200 
99-99: §7,0°375052 


130 | 99,33-1 110.3 79842 
132 [100+ 4.430.384576 


134 


TOO 35-450 389252 
136 |tol. §.48 
138 1017.35.22 
T40 1102. 4.1519 


0.393868 
0.398428 
0:4029230 


Med, 


y 


92.12.1410.318060 | 
| 92-54. 410.323587 


_ cn Aad MY PS 


 £ 1ggliz2,11.58}0.5c7 42) 


| dng. @ | hogar. 
} per ibelio} pro dift. 
+. | a ole, 


i O- er. ae 
# 142/102. 102.32. 2..4.119.407380 
1441103 00.3119.4117 8s 
146,503. 2704 749-416 132 | 
f 148:103.54.3 10 420430 
i 150}t0% 20.43) alan 


ae E 


ner3 To, see ape ah 
116.39. 749-559538 
117. 6,28109565199 
117.33. 27/0 570762 


{ 154] O51 L, 33 On 433012 
156/105. = 16}>. ries 


f 162 ime. 47.47 loadougd | 
| 107. 10.44]o 453060 
[07.33.17 {99456936 


11937 5610.597252 
120. 1. 6/0 602301 


172 rk 38. 37 \0. 468318 
| £74|108.59. 29|0-¢7 2080 


8 }r20645.52/0 612174 

1120. 7.3¢]0.616998 
{27 28 30/0.621750 
> f42T. 121.49 22]0-626438 


] 178|109. 40. 400.479340 
110 co. 4¢ 0:482937 
t 18011 10.20.20|0.486498 
| 134/110. 39.4 Foe4 0022 
F 186|t 10.5 8-44]0-493512 
IQSILLT.17+2810.496965 | 
| Lgo| 1143 5+55|0.5 00384 | | 300 5 Ge PRED 4 
| £92|t11.54-05]0,503769 || 3 


f 196]112.29.34j0-5f04q1 
1 193)142.46.55/0.513729 
200i 13. 4-colo 5 eoet 


eae RT See 


—Mifcellanea Curiofa, 1X 


Med) Ang. @\ Logar. | Med.[ Ang.a | Logar. 
mot, | peribelio.| pro dift peribelio.| pro diff. 
——|———| 4 Sole. —| 4Sole 
3 gr. gr oon 


360 127.25. 60-708 1o4 
370|123. 2.33'00716976 
390 128,35-3810.725606 
390|129. 7.27.0+734006 
plea cd acl 
“Alol|!30. 7:34l0.750160 
420\130-36+ 210.757930 
430|131. 3.30|0.765516 
4.4:c}131-30- 219,772918 
4501131-55+41\0.730148 
460]! 32+20.30]05787216 
470|'32-44-3210,794122 
48 0|133- 7-5, 6.800882 
490|!33+30.2.|0.807494 
§.00|133+52.2 ,jo.813969 
§ 2c|134-34+18]0.8265 22 
540|135-14+ 0]0.838600 
§ 60|13 5+51.28]0.850187 
§80|136.27- 6]0.861359 
60¢ [37-00-57 0.872155 
620|137.33-13]o 982575 
640]138> 3+55|o0892649 
660,138.33:21lo.902401 


141-49+2410.970836 
142.10.00]0.978397 
142.29.5610.985771 } 
142.49+1010.992970 
1430 7.48 o.Ico000 
1143+25.5 1|1,006871 : 
143 43 2111.013586 
144.00.18}t.0201 55 
14.4216.46]1.626583. 

144.3 2.46/1.032876 
149 26. 811.158188 
1§2+26.1511.246058 
15.4+32-2017.313703 
156. 7.27|1.368678 

157-22.49)/1+414974 
158.24.36]1.45495¢ 
199 16.36]1 490125 
160, 1 Ja}t.g21e21 
160.40. §11.549874 
fObt4 aglt575718 
161.45 0Olr 599460 
162.12.34/1 621417 
162.37.34|1.641838 


680,139. 1.29'0.911866 163 .00.23|1 660922 
“Foor 39'28:256-921012 1163 21420 1.678834 


ee eee? 
| 740140019: 5 0.930549 163.58.38!1 711662 
: 7601140.42.56 0.946951 164.15.2011.726784 

78014.1.05:55 0.955124 ||50000 |170.52. 0]2.197960 
Soa r4r 2k. 3 0.063082 1] ro0coclI72.45.44'2.399655 


163 40.4211 695708 


B 2 The 


ra Maifcellanea Curiofa. © 


The Conftruction and Vfe of the 
general Table. 


‘As the Planets move in Elliptick Orbs, fo 
do the Comets in Parabolick ones, having the 
Sun in their common Focus, and defcribe equal 
Area's in equal Times. But now becaufe all 
Parabola’s ave fimilar to one another, therefore 
if any determinate Part of the Area of a gi- 
ven Parabola, be divided into any Number of 
Parts at Liberty, there willbe a lke Divifion — 
made in all Parabola’s, under the fame Angles, 
and the Diftances will be proportional : And 
confequently this one Table of ours will ferve — 
for all Comets. Now, the Manner of the 
Calculation of this Table is thus: In the Fig. 


Let S be the Suz, POC the Orbit of a Comet, 
P the Perihelion, O the Place where the Comet 
is 90 gr. diftant from the Sun, C any other 

Place. Draw the Right Lines CP, CS, and 
makeST, SR, equal to CS; and then having © 
drawn the Right Lines CR, CT, (whereof 
the one isa Tangent, and the other a Perpen- 
dicular to the Curve) let fall CQ  perpendicu- 
lar to the 4x PSR. ie es aa 

Te es easy Now, 


Mifcellanea Curiofa: Fr) 

_ Now, any Area, as COPS, being given, *tis 
requir’d to find the Angle CSP, and the Di- 
ftance CS. From the Nature of the Para- 
bola RQ is ever = 2 the Parameter of the Axisy 
and confequently if the Parameter be put = 2, 
then RQ = 1. Let CQ=z; then PQ fhall = 
z zz, and the Parabolick Segment COP=122%- 
But the Triangle CSP will=4<, and fo the 
_Mixtilineal Area COPS=# 2’|-4 z=, whence 
zi--3 2-124. Wherefore refolving this Cu- 
hical Equation, z or the Ordinate CQ. will be 
known. Now, let the Area OPS be propos’d 
to be divided into 100 Parts; this Area iss. of 
the Square of the Parameter, and confequent- 
ly 12-ais that Square—4. If therefore the 
Roots of thefe Equations z*+3 z = 0, 04:0,08: 
6,12: 0, 16, &c. be fucceflively extracted, 
there will be obtain’d fo many z or Ordinates 
CQ refpectively, and the Area SOP will be di- 
vided into too Parts. And in like manner is 
the Calculus to be continued beyond the Place 
©. Now the Root of this Equation (fince RO 
is=1) is the Tabular Tangent of the Angle 
CRQ, or! the Angle CSP, and fo the Angle 
CSP is given. And RC, the Secant of the fame 
Angle CRQ, is a mean Proportional between 
RQ or Unity, and RT, which isthe Double of | 
 §G, as is plain from the Conicks, But if SP be put 
1 and fo the Latws Reftum — 4 (asin our Ta- 
ble) then RT will be the Diftance fought, vz. 
the Double of SC in the former Parabola. Af- 
- ter this manner therefore, I compos’d the fore- 
going Table, which ferves to reprefent the 
Motions of all Comets: For hitherto there has 
been none obferv’d, but comes within the Laws 
of the Parabela. , 


Ie 


14 WhifceHanea Curiofa, 

It remains now, that we give the Rules for 
the Calculation, and fhew the Way of deter-. 
mining the Place of a Comet feen, by thefe 
Numbers. The Velocity of a Comet moving in a 
Parabola, is every where -to the Velocity of a Pla- 
net defcribing aCircle about the Sun, at the fame 
Diftance from the Sun, as \/ 2 to I. as appears 
from Cor. 7. Prop. 16. Lib. 1. of the Princip: — 
Phil. Nat. Math. Vf therefore a Comet in its 
Perihelium wére fupposd to beas far diftant 
from the Sun as the Earth is, then the Diurnal 
Area which the Comet wou’d defcribe, wou’d 
be to the Diurnal 4rea of the Earth, as {/2 to 
1. And confequently, the Time of the Annual 
Revolution, is to the Time in which fuch 
a Comet wou’d defcribe a Quadrant of its 
Orbit from the Perihelium, as 3.14159, Ces 
(that is the Area of the Circle) to 4/8. There= 
fore the Comet won'd defcribe that Quadrant 
in 109 Days, 14 Hours, 46 Minutes; and fo 
that Parabolick Area (Analogous to the Area 
POS) being divided into 100 Parts, to each 
Day there wou'd be alotted 0.912280. of thofe 
Parts; the Log. of which, wz. 9.960128, is 
to be kept for continual Ufe. Byt then the 
Times in which a Comet, at a greater or lefs Di- 
fiance, wowd defcribe fimilar Quadrants, are as 
the Times of the Revolutions in Circles, that is, in 
the Se/quiplicate Ratio of the Diftances: And 
fo the Diurnal Area’s, eltimated in Centefimal 
Parts of the Quadrant (which Parts we put for 
Meafures of the mean Motion, like Degrees) 
are in each, in the Sub/e/quialtera Proportion 
of the Diftance from the Suain the Perihelion. 


Thefe 


— MifceHanea Curva. 1g 

Thefe neceffary Things premis’d, let it be * 
proposd to compute the apparent Place of aay 
one of the mention’d Comets, for any Gives | 
Time. Therefore, | | 

1. Let the Sun’s Place be had, and the Log, of 
ats Diftance from the Earth. : 

2. Let the Difference between the Time of the Pe- 
rihelion, aad the Time given, be gotten, in Days and 
Decimal Parts of Days. Tothe Log. of this Num- 
ber, let there be added the conftant Log. 9.960128, 
and the Complement Arithmetical of the 2 of the 
Log. of the Diftance in the Perihelium from the Sun 
The Sum will be the Log. of the Mean Motion, to be 
fought in the firft Column of the General Table. 

3. With the Mean Motion let there be taken the 
correfpendent Angle from the Perihelium, zz the 
Table, aad the Log. for the Diftance from the 
Sun: Then in Comets that are Dirett, add, and 
in Retrograde ones fubjtratt , if the Time be after 
the Perihelium, the Angle thus found, to or from 

the Piace of the Perihelion ; or in Direct Comets, 
 fubfirat , and in Retrograde ones, add; if the 
Time be before the Perihelion, the forefaid Angle 
to or from the Place of the Perihelion; and fe 
we {ball have the Place of the Comet in its Orbit. 
. And to the Log. found for the Diftance, let there 
be added the Log. of the Diftance in the Perihe- 
lion, aud: the Sum will be the Log. of the true 
Diftance of the Comet from the Suu. 

4. The Place of the Node, together with the Place 
of the Comet in its Orbit, being given, let the Di- 
 flance of the Comet fromthe Node be found , then, 
the Inclination of the Plane being given, there will be 
given alfo (fromthe common Rules of Trigonometry) 
the Comet’s Place reduced to the Ecliptick, the Incli- 

nation or Hleliocentrick Latitude, andthe Loz. of the 
curtate Diftance. Ce 
5. From 


16 Mifcelanea Curiofa. ik 
5. From thefe Things given (by the wei fame 
Rules that we find the Planets Places, from be ag! 
Place and Diftance given) we may obtain the Ap- 
parent or Geocentrick Place of the Comet, toge- 
ther with the Apparent Latitude. And this -it 
may be worth while to illuftrate by an Exame 
ple or two. sea | 
ExameveE I. 
Let it be requir'd to find the Place of the 
Comet of the Year 1665, March 1°, 7", 
oo', P. M. London. That is. 96%, 19°, 


Novemb. 2h, Ar, 52". 


Log. Dift. Perihels oc. o7 1044 
Log. Se(quialt. o 916566 
: : 9: 960128 
Log. ‘Temp. te 985862 

f Log. Med. Mot. 1.929424 
Medius Motus 85.001 
Perihel. SU 10. 41. 45 
Ang. Correlp. 83. 38. os— 


Comet. inOrb. GB 37+ 3° 20 
' Afcend. Nod. TL 2%. 14: 00 


Com. a Nodo (34. 1O- 40 
Red. ad Eclip. 22 19+ OF 
Com. Helioc. © i ee 
Incl. Bare o37 ize 46. 50 
Log. pro dif. O. 255369 
Log. Perihel. QO, O11044 
Co-fin. Incl. 9g 990754 


Log, dift. Curt. 257197 
Lor. di O >. 997918 
© xX 


21+ 44. 4§ 
Com. Vifus VW a9. 18. 3° 
Lat. Vila 8. 36 15 
' EXAMe 


5 i eal 
J = Ge ae = 


81, after the Perihelion, which happen’ 


La ie be requir'a to 
met of the Year 1683, 
P.M. London: Or, 1 


That 15, 214, 108, 


Mifeclanee Curiofa 


Examecre Il, 
find the Place of i Co 0- 


helion, 


fini. 


the 
fo chavit Wa foutid if be"9 


Lae 


foc mo deomy Nuts, 25 


Log, diff. Perihel, 9. 


748343 


Log. SeGuialt. 9. 622514 
Comp. Arith, ©. 377486 
| é 9-.950128 
Log. Temp. I+ 310723 
Log. Med. Mot. cass} 648337 
Medius Motus 44. 498 
:: ee aa | 25. 29: 30 
Ang. Correfp. 56. 47. 20— 
Comet. in Orb. Fs 28. des ns 
Nod. Defcend. Fe ee 23. 00 
Com, a Nodo 35° 19. 10 
Red. ad Eclip, - 4.48. 30 
Com; Helio. %€ 28.11. 30 
Ancl. Bor, 35+. 2» a0 
Log. pro dift; O- 111336 
1 Log, Perihel. 9: 748343 
“Ce: fins Incl, gies AE old 
AED Hog difk Curt, g. 772866" 
HL SOs) dif) OX 0958101606 194541 
Wi 13:5 Locus Sy PDT A Ags 25 Oy 
te eArlitle So...., 
Lat. Vor. | 28 2 90 


xam) ple, “twas obferwd. (at. London) 


tiapp lied to the Secand St taro 


ae Noi 


17 


July PME Sued Ue 
3", 40! Equat. Time. 
50’ after the Peri- 


“At the, Tnftant re Tine: ‘Specified’. in pin 


) that. 


ries-> 


hetly, 
and 


* 


i8 Mifcellanea Curiofa. | 
and 3! to the Eaft, according to Mr. Hook’s Ob- 
fervation. But at that of the Second Example, 
Imy felf (near London, with the fame Inftru- 
ments whereby I formerly obferv’d the. Sou-) 
thern Conttellations) found the Place of the 
Comet.to be %, 5°, 11/', and 28°, 52! North 
Latitude, which agreed exaétly with the Ob- 
fervation made at Greenwich almolt thé ve1y 
fame Moment. | | bOT La 
As for the Comet of the Year 1680, which 
came almoft to the very Saw it felf (being in 
its Perihelion, not.above } of the Semi-Diameter — 
of the Sun diftant from the Surface of it) fince 
the Latus Reftumisfo very fmall, could hardly 
be contained within the Limits. of the General 
Table, becanfe. of. the exceflive Velocity of 
the Avean Motion. Therefore in this Comet, 
the beft Way is Cafter the Atean Motion is - 
found) to get from thence (by the Help of the 
foregoing Equation <’- 32 =-* of the Mean 
Motion) the Tangent of Half the Angle from 
the Perihelion, together withthe Log. for the 
Diftance from the Sun. ‘Which Things being 
given, we are to proceed by the fame Rules, 
as in the reft. vk | 


After this Manner therefore, the Aftrono- 
mical Reader tay examine. thefe Numbers, 
which I have calculated, with all imaginable 
Care, from the Obfervations 1 have met with. 
And I have not thought fit to make them pub- 
lick before they have been duly examin’d, and 
made as accurate as "twas poflible, by the Study 
of many, Years. 1 have publifh’d this Speci- 
men of Cometical Aftronomy, as a Prodromus 


of a defigned future Work, left, “happening 
: (Oy Lo tae ait ye Wis CRY 2. £9 


* 


Mr|celanea Curiofa. 19 
to die, thefe Papers might be loft, which 
every Man is not capable to retrieve, by rea- 
fon of the great Difficulty of the Calculation. 

_Now, it may not be amifs to put the Reader 
in mind, That our Five firft Comets, (the 
‘Third and Fourth obferv’d by Peter Apian, the 

Fifth by Paulus Fabricius) as alfo the Tenth feen 
by A4e/tiin, if 1 miftake not, in the Year 15960. 
are not fo certain as the reft;. for the Obferva- 
tions were made neither with fit Inftruments, 
nor due Care, and uponthat Account are dif- 
agreeing with themfelves, and can by no means 
be reconcil’d with a regular Computation. The 
Comet which appear’d in the Year 1684. was 
only taken Notice of by Blanchinus, who obfer- 
ved at Rome: And the laft, which appear’d in 
the Year 1698. was feen only by thofe at Pa- 
viz, who deterimin’d its Courfe in a very un- 

common Way. This Comet was very obfcure; 
and, altho’ it movd fwift, and came near e- 
nough our Earth; yet we, who are wont to 
be curious enough in thefe Matters, faw no- 
thing of it. For want of Obfervations I have 
left out of the foregoing Catalogue, thofe Two 
remarkable Comets which have appear’d in this 
our Age, one in November, in the Year 1689 the 
other in February in the Year 1702. For they di- 
recting their Courfestowards the Southern Parts 
of the World, and being {carce conf{picuons here 
in Europe, met withno Obfervers capable of the 
Bufinefs. But, ifany one fhall bring from Jrdia, 
or the Southern Parts, an accurate Series of re- 
quifite Obfervations, | will willingly fall to work 
again; and undergo the Fatigue of reprefent- 
ing their Orbits in Numbers, as 1 have done 
eee ) 
crear. C 2 | By 


20 Mifcelanea Curtofa. = 

By comparing together the Accounts of the 
Motions of thefe Comets, “tis apparent, their 
Orbits are difpos’d in no manner of Order 5 
nor can they, as the Planets are, be ne 
hended, within a Zodiack, but move. indiffe- 
rently every Way, as well Retrograde as Di- 
rect ; from whence it is clear, they are not 
carry’d about or mov’d in Vortices.. Moreover, 
the Diftances in ‘their Perihelium’s are fome- 
times greater, fometimes lefs ; which makes 
me fufpect, there. may be a far greater Num- 
ber of them, which moving in Regions more re- 
mote from the Sun, become very obfcure;, and 
wanting Tails, pafs by us unfeen: y caus 

Hitherto I have confider’d the Orbits of 
Comets as exactly Parabolick; upon which 
Suppofition it wou'd follow, that Comets be- 
ing impelld towards the Sun by a Centripetal 
Force, defcend as from Spaces infinitely di- 
ftant, and by their Falls acquire fuch a Velocity, 
as that they miay again run of into the remo- 
teft Parts of the Univerfe, moving upwards 
with fuch a perpetual Tendency, as never to 
return again to the Sun. But: fince they ap- 
pear frequently enough, and fince none of them 
can be found to move with an Hyperbolick 
Motion, or a Motion fwifter than what the 
a Comet might acquire by its Gravity to the 
San, ’tis highly probable they rather move in 
very Excentrick Orbits, and make their Re- 
turns after long Periods of Time: For fo their 
Number will be determinate, aad,. perhaps, 
not fo very great. . Befides, the Space between 
the Sun and the fix’d Stars is fo immenfe, that 
there is Room.enough for a Comet to revolve, 
tho’ the Period of its Revolution be vaftly.long. 

se NOW» 


MifceHanea Curtofa. 21 
Now, the Latw Reflum of an Ellipfis, is to the 
_ Latus Retium of a Parabola, which has the fame 
- Diftance in its Perihelium; as the Diftance in 
the Aphelium in the Elipfis, is to the whole 
Axis of the Elipfis. And the Velocities are 
in a Subduplicate Ratio of the fame: Where- 
fore in very Excentrick Orbits this Ratio comes 
very near to a Ratio of Equality ; and the very 
{mall Difference which happens on Account of 
the greater Velocity in the Parabela, is eafily 
_compenfated in determining the Situation of 
the Orbit. The principal Ufe therefore of 
this Table of the Elements of their Motions, 
and that which induced me to conftruct it, is, 
That whenever a new Comet fhall appear, we 
may be able to know, by comparing together 
the Elements, whether it be any of thofe which 
has appeard before, and confequently to deter- 
- mine its Perjod, and the Axis of its Orbit, 
and to foretell its Return. And, indeed, there 
are many Vhings which make me believe 
that the Comet which pian obferv’d in the 
_ Year t93r. was the fame with that which 
Kepler and Logomontanus took Notice of and 
defcrib’d in the Year 1697. and which I my felf 
have feen return, and obferv’d in the Year 1682. 
All the Elements agree, and nothing feems ta 
contradic thismy Opinion, befides the Inequali- 
ty of the Periodick Revolutions: Which Inequa- 
lity is not fo great neither, as that it may not be 
- OWing to Phytical Caufes. For the Motion of Sz- 
surmis fo difturbed by the reft of the Planets, e- 
{pecially Fupiter, that the Periodick Time of that 
Planet is uncertain for fome whole Days to- 
gether. How much more therefore will a Co- 
met be fubjeé to fuch like Errors, which rifes 
 Seuoee ee ale 


a2  Mifcellanea Curiofa. 
almoft Four times higher than Szeurz,and whofe 
Velocity, tho’ encreafed but a very little, would 
be fufficient to change its Orbit, from an Ellip-- 
tical to a Parabolical one. This, moreover, 
confirms mé in my Opinion of its being the © 
fame ; that in the Year 1456. inthe Summer 
time, a Comet was feen pafling Retrograde 
between the Earth and the Sun, much after 
the fame Manner: Which, tho’ no Body made 
Obfervations upon it, yet fromits Period, and 
the Manner of its Tranfit, 1 cannot think dife 
ferent from thofe I have juft now mention’d. 
Hence I dare venture to foretell, That it will 
return again in the Year 1758. And, if it 
fhould then return, we fhall have no Reafon 
to doubt but the reft muft return too: There- 
fore Aftronomers have a large Field to exercife 
themfelves in for many Ages, before they 
will be able to know the Number of thefe many 
and great Bodies revolving about the common 
Center of the Sun; and reduce their Motions 
to certain Rules. I thought, indeed, that the — 
Comet which appear’d in the Year 1532. might 
be the fame with that obferv’d by Heveliusin the 
Year 1661. But Apian’s Obfervations, which are 
the only ones we have concerning the firft of 
thefe Comets, are too rude and unskilful, for 
any thing of Certainty to be drawn from them, 
in fo nice a Matter. I defign to treat of ail. 
thefe Things ina larger Volume, and contribute 
my utmoft for the Promotion of this Part of 
Aftronomy, if it fhall pleafe God to continue 
my Life and Health. a chtsar ued o 
In the mean time, thofe that defire to know — 
how to conftruct Geometrically the Orb of a 
Comet, by Three accurate Obfervations given, 
, may 


} 


WMhi|cellanea ib eae 


“may find it at the End.of the Third Book® of 
‘Sir [aac Newton’s Principles of Natural Phi- 
lofophy, entituled De Syflemate Mundt, in the 
‘Words of its renowned Inventor. Which 
“have fince been more fully. explained by my very 
“worthy Collegue Dr. Gregory, in his Learned 
Work of Aftronomia Phy fic ica & Geometrica. 

One Thing more perhaps it may not be im- 
proper or unpleafant to advertife the Aftrono- 
mical Reader; That fome of thefe Comets 
have their Nodes fo very near the Annual ae 
‘of the Earth, that if it fhall fo happen, t 
the Earth be found in the Parts of her Gi 

“next the Node of fuch a Comet, whilft the.Co- 
met pafles by; as the apparent Motion of the 
Comet will be incredibly fwift, fo its Parallax 
will become very fenfible ; and the Proportion 
thereof to that of the Sun will be given. Where- 
fore fuch Tranfits of Comets do afford us the 
very beft Means, though they feldom happen, 
to determine the Diftance of the Sun and 
_ Earth: Which hitherto has only been attempt- 
ed by AZars in his Oppofition to the Sun; or 
elfe Venus ne Perigao , whofe Parallaxes though 
triple to that of the Sun, are fcarce any ways 
_ to be perceived by our Inftruments , whence 
we are ftillin great Uncertainty in that Affair. 
This ufe of Comets was the ingenious Thought 
of that excellent Geometrician Mr. Nicolas 
Facio. Now the Comet of 1472, had a Pz- 
rallax above Twenty times greater than the 
Sun’s. Andif the Comet of 1618, had come 
down, about the Middle of March, to his de- 
fcending Node: Or if that of 1684, had arr‘-_ 
ved a little fooner at its afiending Node; 


they would have been yet much nearer the 
Earthy 


24 Mifcelanea Curiofa. 

Earth, and confequently have had more nota- 
ble Parallaxes. But hitherto none has threaten’d 
the Earth with a nearer Appulfe, than that 
of 1680. For by Calculation I find, that No- 
“ vemb. 11°, 15, 6', P. AZ, that Comet was not 
above the Semi-diameter of the the Sun to 
the Northwards of the Way of the Earth. 
At which Time, had the Earth been there, 
the Comet would have had a Parallax equal 
to that of the Moon, as I take it. ‘This is 
{fpoken to Aftronomers: But what might be 
the Confequences of fo near an Appulfe; or 
-of a Conta& ; or, laftly, of a Shock of the 
Cceleftial Bodies, (which is by no means im- 
poflible to come to pafs) I leave to be dif- 
_cufs'd by the Studious of Phyfical Matters. 


25 


Geometrical Differtation 


| Concerning iiss ters nants 
RAINBOW: 
IN. 

Which (by a dire€t Method) is fhewn 

' how to find the Diameter of each 

_ Bow, the Proportion of the Refraction 
being given: Together with the Solu- 
tion of the Izverfe Problem, or how 


to fend the Ratio of the Refraéction, 
the Diameter of the Iris being given. 


By Ep. Hatrey, F.R.S. 


of LL the Writers of Natural Hiftory, 
| have particularly defcribed the Rain- 
tL \ bow (a Meteor fo remarkable for its 
fair Colours) and given an Account of the 
Caufes of it. And the Ancient A4tholocifts, 
from its wonderful Form and Appearance, 

me thought 


96 Mifcellanea Curtofa. 

thought fit to give it the Title of Thaumanti, 
or the. Child of Wonder , and placing it in the 
Number of the Goddeffes, attributed to it the 
Office of a Meffenger between the Celeftials 
and mortal Men; which Fable, perhaps, owes 
its Original to Gevefis, Ch.9. V.13. i 
Thofe that attentively confider’d the Phe- — 
nomena of the Rainbow, always found, that 
the Sun’s Rays reflected by a Watery Cloud, 
came to the Eye under a certain Angle; from 
whence arofe the Arch, or Circular Figure of 
it. But as for the Caufe and Reafon of the 
Colours, as alfo of the’ Magnitude of the 
Angle, by which we conftantly find it diftant 
from the Point oppofite ro the Sun; thefe were 
Things, that a long while, and very greatly 
perlex’d, as well the A/oderus, as Ancients. 
Neither did they doany thing to the Purpofe 
herein, till the Famous Monfieur Des Cartes 
making ufe of the Mathematical Sciences, 
fhew’d by feveral Examples, that more ftrict 
and clofe Methods of Reafoning might and 
ought to obtain, even in our Management of 
thofe Phyfical Speculations. Amongft other 
things (tho’ it muft be own’d that herein he 
had fome Light, from the Learned Antonio de 


Dominis, Arch-bifhop of Spalato) he explain’d — . 


the Theory of the Rainbow. And having dif- 
cover’d the Laws of Refraction, he clearly de- 
monftrated, that the Primary Ir was nothing 
elfe, but the Sun’s Image reflexed from the 
Concave Surface of innumerable Spherical 
Drops of Rain ; and that with this Condition, 
that thofe Rays that were parallel at their 
Incidence, were not loft or diflipated by the 
Reflexion, and the Two Refrattions (one at the 
age . | la- 


e 


Mifcellanea Curiofa. 27 
Ingrefs, and the other at the Egrefs) but fell 
(and that alfo parallel) on the Eye. That the 
_Rays were tingd with Colours by thofe Re- 
fractions, after the fame manner as we fee they 
are bya Gla/s Prifme. That the Secundary Iris 
is produced, after the fame manner, by the 

Rays that fall more obliquely, only here are 
Two Reflexions, before the Sun’s Rays (which 
when refracted a Second time proceed parallel 
to the Eye) emerge out of the Drops of Wa- 
ter. Further, that the Magnitude of each Jris 
depends upon the Degrees of the Refraction, 
which is different according to the Nature of 
each tranf{parent Solid or Liquid. ; 

And fuppofing the Proportion of the Sines 
of the Angles of Incidence to the Sines of the 
refracted Angles, to be in Water, as 250, to 
187, he determin’d the Semi-Diameter of each 
Iris, agreeably to Obfervations, viz. that of 
the Primary Ir, 41°. 30'. and that of the 
Secundary, 51°. 54'. By which he did not fo 
much confirm the Theory it felf, which was 
_ demonftrated from other Principles, as the 
— Truth of the fore-mention’d affumed Proportion, 
(viz. that of the Refraction.) But for thefe 
Things, the Reader may confult the 8th Chap- 
ter of Cartes’s Meteors, whither I refer him. 

But now Cartes (who ufed an indire& and 
tentative Method in determining thefe Angles) 
did not feem clearly to apprehend the Ealinefs 
of the Problem he had propofed to himfelf. 
And becaufe none (that | know of) fince him, 
has handled the fame Argument more fully; 
and alfo fince fome have mifunderftood what 
Cartes did, committing very great Paralogifms, 
in fome Books (fince his time) which ao 

larly 


28 | Mifcellanea Curiofa, 


larly sindbis to explain the Phenomena of 


the Rainbow; I was’ willing to fupply- what 1 _ 


thought was ” wanting in this Dodrine, and 
from the Proportion of the Refrattion given, Geo- 
metrically to determine the Angle of its Di- 
ftance from the Point oppofite ro the Suw: Or 
contrarywife, from the Irs given, to determine 
the refractive Power of the Liquid. 

What the Celebrated Mr. Newton has done 
upon this Head, the Reader will find (with 
much greater Advantage) i in his Book of Light 
and Colours, when he fhall think fit to be- 


ftow thofe excellent Difcoveries upon the Pub- 


lick. 

But to proceed. ?Tis plain from what Cartes 
has demonftrated, that the Primary Iris is 
form’d by fuch Rays of the Sun, where the 
Excefs of Two refratted Angles, above one 
Angle of Jacidence, is the Greateft of all fuck 
Exceffes poffible. And that the Secondary Ives is 
form’d by thofe Rays only, where the Excefs 
of Three refrated Angles, above one of Inci- 
dence, 1s in like manner the Greateft. And fo 
we may goon toa 3d, 4th, or any other Is, 
which are form’d, where the Rays emerge af- — 
ter 3, 4, 0Fr more Reflexions. Bat thefe can 

never be feen in the Heavens, becaufe of the 
sun’s Light which is ftill more “and more debi-. 
litated by each Reflexion and Refraétion ; 
Whence it comes to pafs alfo, that the Secon- 
dary Ive, is painted with Colours, fo. much 
faiater than the Primary one.“ But in all thefe 
the general Rule is, that the Excefs of 4, or 5, 
or more refratted Angles, (viz. the Number af 
Refiexions being: increafed by Unity) above one 

vingle of Incidence, w% of all the Greatelf. 
Now: — 


Mifcellanea Curiofa. 29 © 
Now this greate/? Exce/s doubled, is always 
the Diftance of the Jris from the Point oppofite 
to the Sun, when the Number of Reflexions is 
uneven. But if that Number be eve, then the 
Double of that greateft Angle, is the Diftance 
of the Iris from the Sun it felf, viz. in the 2d, 
4th, oth, Gc. Iris. All thefe Things are ei- 
ther purely Cartefizs’s, or elfe eafily follow 
from his Writings in the foremention’d Place. 
But now to obtain thofe greateft Exceffes, 
having the Refra@ion of any Liquor given ; 
tis to be obferv’d, that the Excefs of Two 
refraded Angles, above one of Incidence, is 
there the Greate/?, where the momentancous In- 
crement of the Angle of Incidence is exa@ly 
double of the momentaneous Increment of the re- 
fracted Angle.. And:that the Excefs of Three 
refracted Angles is there the Greate/?, where 
the Increment of the Angle of Incidence is 
triple the Increment of the refracted Angle; — 
and fo of the reft. And this is fufficiently 
evident of it felf: But asfor the Angles, we 
may obtain them by the Heip of the following: 
eid dade muff therefore be demonftra- 
ted. . 


Ewa 


20 WVhifcellanea Curiofa. so 


LEM™ A. 


The. Legs. of any plain Triangle continuing ; 

af the Vertical Angle be au mented or 
diminifb’d, by an Angle lee than any 
Angle affign’d , the Momenta or Inftan-- 
taneous Mutations of the Angles at the 
Bafe, are to one another reciprocally, as 
the Segments of the Bafe. | 


At Fig. 1. Plate 3. fuppofe the Triangle 
ABC, whofe Vertex is 4, its Legs AB, AC, 
and Bafe BC, upon which let fall the Perpendi- 
cular AD. .Then let the Angle BAC be in- 
creafed by the Indivifible Momentum CAc, and 
let the Lines Bcd, c D be drawn, which dif- 
fer, in Imagination only, from the Lines BCD, 
CD. fay, that the Aomentum of the Angle 
ABC (viz. CBe) is to the Afomentum of the 
Angle ACB or ACD, as CDto BD, that is 
reciprocally as the Segments of the Bafe. 


DEMONSTRATION. 


Becaufe the Angle ACD, is the Sumof the 
Angles ABC, BAC, its Adomentum alfo fhall 
equal the Sum of the AZomenta of thofe Angles ; 
that is, it fhall equal CAc-+-CBe. But CAc 
= CDe, fince, becanfe of the right Angle at 
D, the Points A,D,C, c, are all in the Arch 
of aCircle, whofe Diameter is AC: By Eucl. . 
3.9. And confequently the Sum of the Angles 
CBc, CDec (that is the Angle Ded) hall be 
the Momentum of the Angle ACD or ACB. 

But 


Mifcellanes. Curiofa.. 31 
But thofe Angles CBc, Ded, being indefinite- 
ly fmall, are to one another-as their oppofite 
fides, that is, as eD orCDto BD, that is as 
the Segments of the Bafe reciprocally. Q: 


_ If each of the Angles Band C be Acute, the. . 
Lemma will {till (mutate mutandis) be demon- 
- rated after the fame Manner. ~~ : | 
COROLLARY. 
Hence it follows that the Avomenta of the 
_ Angles at the Bafe, are to one another direttly, 
as the T'angents of thofe Angles. | 
By the Help of this Lemma, I will be eafie 
to find the Diameter of any Jris whatfoever 5 
and that either by Calculation, or a Geometrical 
Conftruttion, For taking any tight Line, as 
CA (Fig..2.) let it be divided firft of all in 
D, fo that CA, may be toCD, in the Ratio 
of the Refraction in Water, which is as 250 
to. 187, or more accurately, as §29 to 396. 
Then let CA be divided fo in E, that CE may) 
be to AE, as Unity to the Number of Reflexi-. 
ons, a Ray of the Sun (fit to produce. the Tris 
propofed) undergoes: And upon the Diame- 
ter AE defcribing the Semi-Circle ABE, on 
the Center C with the Radius CD defcribe the 
Arch BD, meeting the Semi-Circle ABE in 
the Point B. Laitly, Drawing the Right Lines 
2B, AB, let CF be let fall perpendicular upon 
AB produced, and EB paralfel thereto. | fay 
then, that CBF is the Angle of Incidence, and 
CAB the Refracted Angle that we enquire af- 
ter, and: which will produce the Js pro- 
eS, aaa D E- 


32  Mafcellanea Curiofa. 
DEMONSTRATION. — 


Becaufe the Triangles ACF, AEB are fimi- 
lar, it will be AF: BF:: AC:EC; that is, 
asthe Number of Reflexions-encreas'd by Uni- 
ty to Unity (by the Conftruttion) and confe- 
quently the A¢omentum of the Angle CBF, will 
be to the Afomentum of the Angle CAF, in the 
fame Proportion (by the foregoing Lemma.) 
But the Sine of the Angle CBF, is to the 
Sine of the Angle CAF, in the Proportion of 
the Sides CA, CB, that is, in the Proportion 
of the Refraction given (alfo by the Conftruttion.) 
Therefore CAF is the Refracted Angle, cor- 
refponding to the Angle of Incidence CBF; 
and their Afomenta are in the Ratio propos’d, * 
wherefore they are the Angles fought. Q.E.D. | 

And now, multiplying the Refracted An- 
gle by the Number of the Reflexions encreas’d 
by Unity, and from the Product fubftraéing 
the Angle of Incidence, we fhall have half the 
Diftance of the Wis from. the’ Sun, if ‘the 
Number of Reflexions be even, or from the 
Point oppofite to the Sun, if that Number be 
uneven, as we have fhewn already. Hence 
we may exhibit (by a Confrattion concife and 
eloquent enough) the Incidencies of all the 
Orders of iris’s, td -any Liquor whofe Refra-* 
ction isknown. For if theLLine AC (FIG. 2,) 
be divided into: Two eqnal Parts at E, into: 
Three equal Parts at ¢, into Four at <, inté: 
Five atv, &c. And on the Diameter AE, ‘Aé,. 
Az, An, be defcrib'd, the Semi-Circles ABE,” 
Abe, Ape, Aun; which are~ all’ interfe@ted cin’ 
the Points B, b, 6, v, bythe Arch DBbéu,;-de= 

Bi ah ferib’d 


Pataca 
Pa =p ee 
es 


Mifcellanea Charcofis igs 


4 -ferib’d on the Center C with the Radius CDo. 
which is to AC, in the given Proportion of 


of the Refracted Angle V 


the RefraGion: I fay then that the Lines 
AB, Ab, A8, Av, will make with the Line 


AG, the Angles CAB, CAb, CA3, CAv, equal 


to the Refradted Angles; and with the re- 
fpective Rayes CB, Cb, C3, Cv, they will 
make Angles equal to the Angles of Inci- 
dence that are required ; viz. ABC (or ra- 


ther its complement to a Semicircle) for the 


Primary Iris, AbC, for the Secondary, ABC, 


for a Third Tri, AvC, for a Fourth, If any 


one has a mind, to find thefe Angles by an 
accurate Calculation, twill follow from the 
fame Principle, that putting the Radius—t, 
and the Ratio of the Refraction as; to s, the 


eee eee 


: Sine of Incidence will be ¥: Si OS aad the 
| 3 


| 355, 
Sine of the Refra&ed Angle V4! fom 
Beit o> 


which Angles proceeds the Primary Iris. For 


the Secondary the Sine of Incidence wiil be 


, - S I 
eae ‘and the Sine of the Refracted 


Bi, 


Angle joel = Fora Third Tris, the Sine 


err eB; 
of Incidence will be V16 oR aed. and the Siné 
f , ig? wes 


1655. rt 
——-—-. Fora 
19rr 15. 


D | | Fourth ; 


eS Pee eee eee Raha hy 
Le 


24. Mifcellanea Curiofa, - 


Fourth Iris, the Sine of Incidence will be 


V25_ +" and the Sine of the Refracted 
24; DAMS. 63 : 


aad oheag and in like manner of 
247r 24 ! : 
thereft. Farther, ’twill be found by Calcu- 
lation, that (taking Cartes’s Proportion) the 
Primary Tris is diftant 41°. 30. from the 
Point oppofite to the Sun; the Secondary, 
g1°.§5- fromthe fame. The Third, 40°. 20. 
and the Fourth, 45°. 33- from the Sun it felf; 
which Jrés’s perhaps were hardly ever feen for 
the reafons before mentioned.  —>_—. 

And thus much may fuffice concerning the 
Magnitude of the Jrides, in the perfpicuous 
Drops of a Fluid, whofe Refractive Power is 
known. It remains that nothing be faid con- 
cerning the Colours, which this Phenomenon 
prefents, with the orders of them in each 
fort of Jris, according to all the poffible Vari- 
ations of the Refraction. ‘ 

And here we muft know efpecially, that 
the Acute and Sagacious Mr. Newton, has 
found by moft clear Experiments, that the 
Rays of Light are not Simple and Uniform,* as 
they iffue out of the Luminous Body, but the pure 
white Light which we fee, confifts of Corpufcles of 
all kinds of Colours, mix’d and hurried with 
a violent Motion, one amongft another.. And 
that the diverfity of the Colours of things 
 arifes, according to the various Difpofitions 
thofe Objects have, to Refract or Reflect this 
or that peculiar kind of Light. Maoh 

The Proof of which is manifeft from Refra- 

: ctions, 


Mifcelanea Curiofa. 35 
tions, in which thefe Species are feparated 
from one another, and the Blue or Purple 
Light, (even in the fame Diaphanous Body) 
is more Refracted than the Ye#om or Red. But 
_ let the Reader confult this incomparable Per- 
fon’s Letters (N°. 80. and the following of the 
Philofophical Tranfattions) from which Speci- 
-men he will be able to judge, how nobly this 
Argument of Light will be managed by him. 
To my purpofe ’tis fufficient, that all kinds 
of Blue Light, are fomething more refrated 
than Red, from which difference arifes the 
Latitude of the Jrides, which is hardly to be 
determined by Obfervation, becaufe of the 
uncertain Limits of the Colours. But by how 
much the Proportion between CA and CD, is 
of greater Inequality, or by how much the Re= 
fraction is greater, fo much the greater is the 
diftance of any Jris from the Sun, and confe- 
quently thofe borders that are remoter from 
the Sun, fhine witha Purple Colour, but thofe 
that are nearer, with an intenfe Red. 

This may always be feen in the Primary 
Jris, which vanifhes in the part oppofite to 
the Sun, if the Sine of Incidence be to the 
Sine of the Refraéted Angle, as CA to CE, _ 
“or as2tor. But if that Ratio be greater, 
there can be no Primary Jris feen at all. i: 

As for the Secondary Iris, ’tis to be noted; — 
that this vanifhes into a Point, in the part 

oppofite to the Sun, when the Ratio of the 


pay ak : nnt 
' Refraction is as 1 to yan —. vs , .or'as.t 


to 0847487... and from thence it returns 
back to the Sum it felf, where it vanifhes, if 
the faid Ratio be as 3 to 1, or as CA to Ce: 

D 2 But 


rk » 3 ; ~ 4 ot ST) AEP RE Pe oe at eee Oe ee 


36 Mifcellanea Curiofa. 
But in the Ratio’s between thefe (fuch as we - 
have in all Fluids known to us, except the 
Air) by how much the greater is the Ratio, 
by fo much is the Js more diftant from the 
Point oppofite to the Sun, or rather from the ~ 
Sun it felf, reckoning the Arch beyond a 
Semicircle. And confequently the Colours 
will feem to be in a different order from the 
| Primary Iris, in thefe returnings, unlefs the 
diftance of the [vides from the Sun, be taken 
in this Sence, which is alfo every where to be 
obferved in the reft. 
The Third Iris is confafed in the part op- 
at to the Sun, the Ratio of the Refraction — 
eing as 1 to,91855--- from thence it re- 
turns. back to the Sun in the Ratio of 1 to 
,68250--- whence again, the order of the 
Colours being reftored,in the Ratio of 4 to 1, 
or CA to Ce, it terminates in the part oppo- 
fite to the Sun. The Fourth Jvs beginning 
from the Sun, in a Ratio of Equality, pafles 
on to the oppofite Point, in the Ratio of 1 to 
,594895--- andthence returns back to theSun, © 
if the Proportion be as 5 to 43 hence again, 
it difperfes*to the Point oppofite to the Sun 
in the Ratio of 1 to ,55337---, within which 
_compafs are included the Refradtions of all 
Fluids that are known. Laftly, The Ratio | 
-being as 5 to 1, or CA toCn, it vanifhes in 
the very Sun it felf; the Colours being every . 
where cnverted to the fight in its return to 
the Sun, as they were ereét in its egref/s from ~ 
It. Hlence, in watery Clouds, the Br/?t and 
Fourth Iris fhew deep red Colours-turned to- 
wards the Sun; but the Second and Third give © 
Purple, But perhaps I may feem too tedious 
“in 


Muifcelanea Curiofa, 27 
in thefe Defcriptions, the Rainbow it felf. bes 
ing no more than a Momentary Phantafm... 

_ But whence ’tis that the different Refra- 
clive Power of Fluids arifes, is a Problem of 
the greateft Moment » and to,be rank’d 
amoneft the Secrets of Nature, not yet. ob- 
vious either to our Sences.or our Reafonings. 
For pure Water amoneft all. Fluids, . does 
leaft of all Refra& the Rays of Light. When 
tis Tinfur'd with Salts diffolved in it, accor- 
ding to its weight and the quantity of Salt, 
it increafes the Refra@ions. . And Corr ofive 
Spirits (which. are much heavier than Water) 
do alfo much more Refra& the- Rays. of 
Light: Nor is it any wonder, fince being 
denfer Bodies, they may eafily be conceived 
fo much the more to obftrué the paflage of 
the Rays. But why there fhould be f great 
a Refraction in Burning Spirits and Oils, efpe-' 
cially in Spirit of Turpentine, or of Wine, {ince 
_ they are Fluids extreamly Light in comparifon 
of Water, and confift very much of fubtle 
fétherial Particles, does. not fo eafily appear’; 
but feems,to. require (in order to the Expli- 
cation of it) a more thorough knowledge of 
the Nature and Texture of Light. 

But. from the diftance (of the Jvs from the 
Sun) giver, to find the Ratio of the Refra- 
ction, is a thing that will give thofe that are 
curious, an occafion of finding the RefraAion 
of any Fluid, accurately and with little trou- 
ble. For if a fmall drop of any tran{parent 
Fluid, be fuppofed to hang at the bottom of 
a {mall Glafs Tube, and the Sun being near 
the Horizon and fhining ftrongly, it be ob- 
ferved under what Angle (with the Poize 


eHIEITD 3 oppofite ~ 


38  Maifcellanea Curiofa, 

oppofite to the Sun) the Colours of the Jris be 

feen in the drop, then the Proportion fought 

_ will be obtained with a little Calculation. It 
is a Cubical Equation, explicable by one only 

Root, by which, from the Primary Iris given, the 

Ratio is computed, wiz. T? 43 T?t—4rrt=o, 

where T is the Tangent of the Angle of Jnci- 

dence requifite, t the Tangent of $ the diftance 
of the Iris from the Point oppofite to the Sun, 

to the Radiusv=1. Whence (according to 

Cardanus’s Rules) arifes this Theorem, viz. 

From the Cube of t fubftratt the Produ of 2tr 

anto the Excefs of the Secant of the fame Arch 

above the Radius; the difference {hall be the leffer 
Cube. The Sum of the fame, adding atrr, will 

be the greater Cube. The Sum of the fides of both 
Cubes, and of t, will be equal to the Tangent of 
the Angle of Incidence, and the half of that, will. 
be the Tangent of the Refratted Angle. From — 
whence the Ratio. fought-is manifeft. 

Kor an Example of this. In adrop of Oi of 
‘Turpentine, the diftance of the Primary Iris; © 
from the Point oppofite to the Sun, is ob- 
ferved to be 25°. 40’. °Tis required to find 
the Ratio of the Refraétion. 


©, 2278063 


t=Tahey \12°i - go. hes 

s=Sec. of the fame.’ = 1, 0256197. ~ 

ttt oe) SO OL a aay | 
pert tT TB ; : Ly 
SE X.2E0. = 05 OLIGIIOS V,- 


The Difference is the lefler Cube Q; 0001495 2 
: whofe fide 0,0530773 . 

The Sum 0, 02349482, Osea Ht, ae 

4trr 0, 91122525. | : 


Re | 
ed 


Greatey 


—  MifceNanea Curiofa. 29 
Greater Cube o, 93472007, whole fide 0, 9777486 
ah : t 0, 2278063 
et ne. liicid. 51°. 32’. 1, 2586322 
2 Beane. Ref. 52°. 11’. 0, 6293161 
_ . Laftly, AsVTT-4' VTT Oe poe 
12168026. Which Proportion comes very 
near to that, which Experience fhews to be 
in Glafs and moft pellucid Solids. The Dia- 
mond indeed, exceeds all tranfparent Bodies, 
- Hot only in refpect of its hardnefs and value, 
but alfo its RefraGtive Power, the Propor- 
tion here being as 5:2, nearly, or more ac- 
curately as 100:41. But of this, perhaps 
more in another place. | 
While I was writing thefe things, that 
_ skillful Geometrician Mr. De Moivre, at my 
requeft, found a like Equation for deter- | 
mining the Ratio, from the Semidiameter of 
the Secondary Iris, given. By which, the Ratio 
is indeed fomething more exadly determined, 
but that Equation being a Biquadratical one, 
the Calculation is not fo ealily performed. 
This Equation is T*-- 4 T? t—2 T? 1r?— 3 
_ r*=0;3 where Tis the Tangent of the Re- 
fracted Angle, t, the Tangent of 3 the di- 
ftance of the Iris from the Point oppofite to 
the Sun, to the Radius r=1. And this Equa- 
tion is of that Form, as to be always expli- 
cable, by an Affirmative and one Negative 
Root, the one and the lefs of which, is the 
Tangent of the Refracted Angle, in the Ke- 
grefs to the Sun, viz. when the Purple Colours 
are nearer to the Sun. The greater Root is 
the Tangent of the Refracted Angie in an 
: 4 Iris 


~ 


4Q Niheallnas Curio! a 


Iris. Lone out. from the Sun, viz ei in m 


a lefs Ratio. An Oil of Turpentir ne, the Pe hl 


af ‘cis | ‘Tris from the. Point oppolite the 
Sun,.. 1s. obferved. to be 81°. 30~ whe ace the 
curious, Reader may find ‘out the ‘Roots 
&, 80822,-- and—2, 98131-- the Tangents of 
the Refraéted Angles. Hencetis computed the 
Ratio of greater Inequality, as 1 to 0, 67! 


fuch as is in Oil of ‘Turpentine. ‘But: ‘from | 


the greater Root comes forth the leffer Ratio, 


as. 1.0 0,.9§40 nearly, fuch as would be in. 


a Fluid, exhibiting. a Secondary. Tri : Of the 
fame Diameter, but which (after the manner 
of the Primary ‘one) fhould look towal rds. the 
Sun with the Red Colours, ia < 

‘Tf.any one has a mind to find inehs ROG 
by a Geometrical Conftruétion, any Parabola 
being given, it is done with fo much eafe, 
that I need not repeat what I have already 
offered. apDA that Head Philofophical Tranf- 
uttions, N. 188. 

Bach of thefe Equations is deduced from 


what has been faid before, and alfo from © 


the Rules for, the Tangents of the Double 
and ‘Treble’ Arch $s “the yap hint of which, 
may be inftead of a Demonftration even fo 


- thofe that are but meanly VaR in iit 


thia oa 


This Difcourfe. being already in the Fifi. 


there came to my hands (by the. means of q 
Friend) a certain Book; whofe .Title was. 


Thaumantiadis Thaumafia , printed cat. Norim- 
berg 1699, nines the Superintendency of AL. 


Sturmius. Ya which the skillful Author feems 
to have laid together whatever is to be found 


of 


2 


Mifcellanea Curiofa. a1 


of this Argument, as well amongft the Af- 
ese as the ~dncient Writers ; fubjoining and 
tCartes'’s, Eckard’s, "Honoratus Faber’ S, 
and Mariott s Calculus. From whence it is plain, 
that the reft added very little or nothing to 
Cartes’s Inventions, building upon the fame Un- 
geometrical and Tentative Methods of Calcula- 
‘tion. But that the judicious Reader may be 
Menfible, what things Ihave performed in the Do- 
Grine of the iris, { would have him read the 
 fore-mentioned Book, and compare it with this 
Difcourfe ; left in putting out thefe things, I 
Soe feem only to have made an unpleafing 
ition of what had been done before. And 
© what waft Use in Aftronomical Matters, this 
Lemma of ours may be, fhall be fhewn upon fome 
other Occafion. — 


B THE 


42 Fre. da,¥ asin 


Rey a Be Pe 
~ ee | 


Stereagrapbi 2 kb Projtion, 


f fj e +6 1 


‘Laid down and Demonftrated. 


. By Fa. Hodg fon, F. RS. 


DEFINITIONS, 


IRCLES deferib’d upon the Surface of 
the Sphere, are either great or fmall, 
Great Circles are thofe which divide the 

Sica of the Sphere into equal Parts; or 
through which, if the Globe be cut by a Plain, 
it’ will be divided equally. 

_ 2. Small Circles are thofe which cut the Sur- 
face of the Sphere unequally ;, or thro’ which, 
if the Globe be cut by a Plain, it will ie a diyi- 
ded i Into unequal Parts. ee 


3. . The 


Mifcellanea. Cuviofa. 43 


_ 3 The Pole of any Circle, whether Great 
or Small, is that Point upon the Surface of the 
Sphere, which is every way equally diftant from 
the Circumference. : 


Whence it follows. 


‘yCorol. 1. That-every Circlesdefcribed upon 
the Superficies of the Globe has 2 real Poles. 
__ And fince every fmall Circle is equi-diftant — 
from fome one great Circle, it follows, 
2. That the Poles of every fmall Circle are 
the fame with the Poles of thofe great Circles, 
to which they ate parallel. a 
_. 3+ Wherefore all fmall Circles parallel to 
each other, have the fame common Pole, 


~ General Definition. 


Conceive the Eye placed fomewhere in the 
Superficiés of the Globe, and at the fame time 
a-Plain-to-cut the Globe, and to ftand at right 
Angles to the Line connecting the Centers of 
the Globe and Eye. . If infinite right Lines be 
imagin’d to flow from the Eye, to every Point 
an the Circumference. of, every Circle defcrib’d 
‘on its Surface, they will trace out upon the 
Cutting Plain what is, called a Stereographick 
Projection of the Sphere. ba «3 


‘Whence, and’ from the firft Corollary of the 
42,2, Definitions, it follows, 


e : Corl, I That the Eye is placed in one of the 
Poles of that great Circle through which the 
Plain pafles, and upon which the Projedion is 


44 Mifcellanes® } 


to be formed which, ‘for Ditinaions Sake> 
is, called the Plain of Projettion ; ‘and the. Pole 
CARTES to the Eye, the remoter Pole,” 

. That the Pole, when projeéted, ‘falls in 
ae Center of the Plain of Projection, 

3. That All great Circles interfedting each o 
ther in the Eye-Point, will, when projee 
“become right Lines, interfecting each: th 1 
the Center or Pole of Projection, ‘inafmucli 
~ they all lye in the fame Plain with the Eye. 

4. That the Poles of every fuch Circle will 
be found in the Circumference of the Plain‘of 
_Projeétion, at 90 Degrees. diftance from ‘ ‘the 
Gircles Interfeétion. | 

5. That the Lines flowing frouf thie Bye to 
any other Circle whatfoever, form a Conical 
Superficies. 

And in order to enquire into their Nature 
and Properties when projected, it is: necellary 

to. premife the two following. Lininia’s, ef v4 


“LEMMA the It. 


If an “ape Cone be cut with a Plain, pa- 
_ rallel to the Bafe, the Section made in the Super- 
ficies of the Cone will be the Circumference of 
a Circle, whofe Center will be found'in the 
right Line, connecting the Vertex of the Cone, 
and Center Of ats’ Bates 


Whence, and from the pelea Definition, it 
follows, ap saci 
Tos 
Corol. 1. That all fmall Circles pavaltel eb 5 the 
Plain of Projetion, will become Cireles in the 
Projection. 


2. That 


Mifcellenea Curiofe. — 45 


soi That.they, will all have one common Cen. 
oter, viz. the Center or Pole of Projection. on 
3. That their common Center, viz. the 
Centre of Projection, will be their common 
Pole. 
20 dae ‘That their Radij or Semi-__ ig. Ie 
‘diameters will be equal to the 
Semi-tangent of their Diftance from the rema- 
» tek Pole of Projection. 

For in Figure 1, fuppofing ¢ the Eye, ab 
(the Plain .of Projection, p its remoter Pole, 
»cand mn, the Circle to be projected; oc equal 
sito gq, will be equal to the Semi-tangent of mp 
or pn, the Diftance of the Circle mm im trom p-the 
03 remater Pole. 


~ LEMMA the Id, 


tl a an inclined Cone be cut with a Plain 3 not 
i elas, to.the Bafe, yet fo that it cuts off a 
Part fimilar to the whole, the Se¢tion made i in 
the Superficies of the Cone fhall be a Circle. 


Whence it follows. 


do That all Circles. whatfoever ( except 
aiff fach as lie in the fame Plain with the Eye, and 
“eine which have been already confidered) tho they 
are not parallel to the Periphery of the Plain 
of Projection, yet become Circles in the Pro- 


i: je@ion.. 


For if, as before, e reprefents Fig. 2, 344: 
the Place of the Eye, ab the Plain 


a » of; Projection, p its remoter Pole, and mn the 


- Circle.to be projected. 
wiT ss Through 


46 Mifcellanea Curiofa, 


ace _ Through 3 n draw nr parallel to. 
Fig. 2, 3,4. “ab, thenis the Angle rae equal to. 

| emn and men, common to both: z 
Wherefore the Triangles’ émn and eny, and 
confequently eoq, are fimilar, and oq a Circle Te by. 
the 2d Lemina. | ss | 


_ Wherefore, a 4: pdt 10 Dios 


Fig. 2, 3, 4. 2. That of all’ the pibnglests: of 

any one of thofe great Circles to” 
be projected, their Centers and Poles will be. 
found in that projected Diameter, which con- 
nects the two InterfeCtions of the Circle to. be, 
projected; and that other great Circle: which. 
a through the Eye, and cuts the Circle to’ 

€ projected at right Angles. 


DEFLN BED Bp 


Which for Brevity’ s Sake i is called biel Pros 
jected Axis: Thus oq is the projected Axis. 
3. That all fmall Circles: will have’ their. 
projected Axis’s in that Line, in which the pro-. 
jected Axis of the great Circle lies, to. which, 


. they are parallel. 


“4 That the Semitangents of the preateft. 
and leaft Diftances of any Circle from the re-. 
moter ‘Pole of Projection, fet off eitlier on. “the. 
fame or contrary fides of the Center of Proje&ti-.. 
on, as the Cafe directs, will give the Interfecti-" 
ons or Extremities of the projected Axis, 
~ 5. That of every great. or fmall Circle. 
within which the Pole of Projection lies, hele, 
Diameter or projected Axis is equal to 
Sum of the Semi-tangents of their great 

an 


—  Mifcellanea Curiofa. 49 
and leaft Diftances .from, the Pole of. Proje- 
» Thus in Fig. 2. and. 3. 0g equal to oc and ¢q 

together, is equal tothe Sum of the Semi-tan- 
gents of the Arches mp pn, the greateft and 
leaft Diftance of the Circle from the remoter 

Pole of ProyeCtion;.....cagatyror io é 

6. That of every {mall Circle without which 
the Pole of Projection lies; its Diameter or 
projected Axis is equal to the Difference of its 
greateft and. leaft Diftances from the Pole of 

ProjeCion. 


_ Thusin Fig. 4. 0q is equal to the Difference 
between ¢q and co, the Semi-tangents of pn, and 
pm, the greateft and leaft Diftances of the Cir- 
cle fromthe Pole of Projection. 

~, That of the a Poles of every great Circle, 
and confequently of all fmall Circles parallel 
to it, that which falls within the Plain of Pro- 
jection will be diftant from the Center by. the 
Semi-tangent.of the Excefs of the greateft Di- 
ftance, of the projected. great Circle from the 
remoter Pole of Projection above a Quadrant, 
or the DeféG of the leaft Diftance from the Pole 

of Projection to a Quadrant. | é 

Thus in Fig.2. d the Pole of the Circle um 
is diftant from the Center by the Space of dc, 
the Semi-tangent of the Arches xp the Excefs 
of pm above a Quadrant, or the Defeé of pr 
to a Quadrant. | 


_ 8. Thatits other Pole will be in the projected 
Axis on the contrary fide of the Centre, and 
diftant from ,it by the Semi-tangent of the pro- 
jected Circle’s neareft Diftance from the remotes 
Pole of Projection, Jeffen’d by a Quadrant.. 


9. Hence 


t 


48  Mifeellanea Curiofa, = 
9. Hence we are taught how to find the in- 
terior Pole of any great Circle, and confequent- 
ly of all {mall Circles parallel to it, by fetting 
of the Semi-tangent of the Compliment of its 
neareft Diftance from the remoter Pole of Pro>- — 
jection in its projected Axis, on the contra- 
ry Side of the Center. with the Interfe- 
ction. , DEES AOE 
10. For the exterior Pole, by fetting of the 
Semi-tangent of its neareft Diftance augmen- 
ted by a Quadrant in the projegted Axis 
from the Center, on the fame fide with the In- 
terfection. lait Be IN hy (hi 


PROPOSITION E._ 


If two Circles cab and bag interfec& each o- 
ther in the Point a, the Angle gab formed by 
them at their Interfection will be equal to the 
Angle bse made by the Radii ab and ac, drawn 
to the Point of Interfe@tion 4. is 
' Conftr. To the Point of Interfection 4, draw — 
the Line fa a Tangent to the Circle gab, and dz 
a Tangent to the Circle hac. fab i 
' Demonjftr. Becaufe the infinitely Fig. 5. 
{mall Portions of the Circles gab | 
and hac do coincede with theTangents fa and da, 
and confequently have the fame Direction ; 
therefore the curv’d lin’d Angle gab is equal to | 
the right-lin’d Angle fad, formed by the Tan- 
gents f2 and da: And becaufe the Angle fabis 
equal to dac, take away from each the interja | 
cent Angle dab, and there willremain the An- 7 
gle bac equal to fad, equal to gab, which was 
to be proved, "8 eee 

PRQ-. 


C2 ox 


PROPOSITION I. 


| The Angles made. by the Circles on the 
Surface of the Sphere, are equal to thofe made 
by their Reprefentatives on the Plain of Pro- 


MR iees sarki - | 

The Reafon of which is evident from the ge- 
neral Definition and laft Propo- : 
fition: For (in Fig. 6.) let e Fig, 6. 
reprefent the Eye, bc the Plain 
of Projection, ope the Angle to be projegted, 
draw pn parallel to bc, pd, and pf, Tangents to 
the Circles pe and po, and continne them till 
they meet the Plain be, in the Line df ; 
Becaufe the. Angle dpm is equal to npm, and 
ie equal to mpm, therefore is md equal to 


Wherefore in the Triangles dmp and fmd are 
are to dm, df common, and the Angles 
fam, fdp both right ; therefore the Angle dof is 
equal to the Angle fmd. Therefore, &'c, 


Whence, and from the firft Propofition, 
it follows, 


- 4. That if every great Cir- Fig. 7. 
cle to be projected (which does | 
not lie in the Plain of the Eye) the Tangent of 
the, Compliment of its Diftance from the Pole 
of Projection fet off in the projected Axis, on 
the contrary fide of the Interfection, will give 
its Centre, 2 | 

_ For en is equal to the Tangent of can, the 
Complement of dac. | 


E 2. That 


_-80 © Méfcellanea Caviofa. 
2, That the Secant of the Complement of 
the fame Diftance will beits Setni-diameter ; 
for an equal to dz is equal to the Secant of can, 
the Complement of dac.... 
~-g. Since wa equal. to. dn is pa ad virsanial 
.. en, it follows univerfally, that the Semi-tangent 
of the Diftance of any great Circle:to bé»pro- 
__ jected. ( that. does not pafs through: the: Eye- 
Point) from the remoter.Pole-of;Proje@ion, 
_ Setoff in the projected Axison.one, fide: of the | 
.. Center, will give. its Interfection 4>“and*the 
..Fangent, of the Complement of the fame Di- 
ftance, fet off them the fame projected:Axis on 
_ the contrary. ts will giveits-Centre. 
cb . In-all fmallCircles which 
. Fig. 8... cut he Periphory. of :the! Plain 
» . © Of ProjeGion-at« right: Angles ; 
annie which is the fame thing, whofe Poles lie in 
. the Gircumference.of.-the Plain of Projection, 
~ that the Secant of the Complement sof their 
_ .Diftances from the remoter Pole. of Projection, 
_ fet of from the Genter. in‘ the- projected Axis, 
__will give their Centers ; for em: is. exiak to) the 
 Secant of pea... 
man nae §inat he Tangent, of the Garis Bilftence 
,, will be the Semi-diameter 5: fors-ma ‘equal: to 
md is the Tangent of pea, or the Arch” pa'the 
Complement of de its Diftance from the Pole 
of Projection. 
6. Since cm is equal to cdand dm, it follows, 
_ that the Semi-tangent of its Diftance from the 
_ Pole of Projedtion, fet off in the projected Axis, 
gives one Interfection; and the Fangentof the 
_ Complement of the farne Diftance,fet off fron} 
the Interfection the. pes ae gives the Centre, | 


PRO: 


: ‘a4 


a ee or 5 se pordy: ye 
» MISMO 


} ; f a. rN ? ‘ ie & : . 4 
Sha GMP. wh r SB! dK ». eX. 
ee , ¢ & 2} _ e i aS § ‘4 bs 
roimsih PROPOSITION HE 
” ioe: ait Se sé x ; Cys 4 M4 e ‘ vt. p 4h eas. j , 


_ If through the remete Polesof = Fig. 9. 
ootwo Circles, two other Circles 
»obedrawn upon the Surface of the Sphere, they 
yi yill cut°off equal Arches in thofe great Circles ; 
»y andilikewife in the finall Circles equi-diftant 
cofrom® thofe Poles through which ‘they paf. 

)Letp be the Pole of the Circles md and rn, c 
‘othe Poie of the Circles ab and qo; pdnob and 
Ipmrqa the Reprefentation of the two Circles 
© palling through the Poles p andc. I fay, ‘ 

1. iOf the great Circlesmd and ab, the Arches 
oimmd andiab. cut off are equal. F's 
je? For'the Arch pdb is equal-to chd, and pma e- 
esqual to cam, and the Angle apb equal to the 
| Angle bea’; wherefore the Triangle apb and mcd 
ncare equal, and confequently ab equal to md. 


19MR €payiiouss 
tl ik Of theleffer Circles, go and rz equally di- 
»/ ftant fromthe Polescand p. I fay, the Arches 
| goandsrn:are equal: For the Arch caq is equal 
to pmr, and cho equal to pdu, and the Angle 
»geo\equalito rpn , wherefore the Triangles qco 
>) andypmiare equal, and confequently the ‘Atthes 
oigovand> ym are equal: q.e.d. 0°. a 


an 


| Whence it follows, 


50) oie’ Thatif through the Pole of any projected 
igreat:Circle, and any Part or Segment thereof, 
oiLinescbe drawn to the Periphery of the Plain 
cn@f Projection, they will cut off an Arch equal 
tothe Segment of the projected Arch. 


82 Mifcellanea Curiofa: 

2: That if through the Pole of any final} 
Circle, Lines be drawn to the Extremities of 
any Segment or Portion thereof, (and con- 
tinued if need be) they will cut off an Arch 
equivalent to: it in that fmall Circle, which is 
parallel to the Periphery of the Plain of Pro-+ 
jection, and as far diftant from the under Poles — 
as the given Circle is diftant from its upper: 


Pole: 


Baa ee pe EEG AD 


Bye 


eee 


“9% 


Se 


ar. 


Soe obate ‘ _— a pei ieee pata . a in S 4 Leb perag Mears 
ale Madi ae : : earenstasireseeats were ayia urges Anam owe 


ST ne, aoe 
meyer nee ny ot 
ae Te 


6 ee et FP rie